2013
DOI: 10.1134/s0012266113020018
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On the asymptotic stability of equilibria of nonlinear mechanical systems with delay

Abstract: We consider some classes of nonlinear mechanical systems with retarded argument. It is assumed that, in the absence of delay, the systems in question have asymptotically stable equilibria. We analyze how the delay affects the stability of these equilibria. The Lyapunov function method and Razumikhin's approach are used to derive conditions under which asymptotic stability is preserved for arbitrary delay values. We suggest a method for stabilizing strongly nonlinear conservative systems by constructing a delay… Show more

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Cited by 6 publications
(5 citation statements)
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“…Let us choose a Lyapunov function for (5) as follows: Vfalse(x,truex˙false)=12truex˙truex˙+normalΠfalse(xfalse)prefix−δtruex˙λprefix−1xtruex˙+εxσprefix−1xtruex˙,$$ V\left(x,\dot{x}\right)=\frac{1}{2}{\dot{x}}^{\top}\dot{x}+\Pi (x)-\delta {\left\Vert \dot{x}\right\Vert}^{\lambda -1}{x}^{\top}\dot{x}+\varepsilon {\left\Vert x\right\Vert}^{\sigma -1}{x}^{\top}\dot{x}, $$ where δ$$ \delta $$ and ε$$ \varepsilon $$ are positive coefficients, λ1$$ \lambda \ge 1 $$, σ1$$ \sigma \ge 1 $$ are powers to be properly selected. Note that the full energy Efalse(x,truex˙false)=12truex˙truex˙+normalΠfalse(xfalse)$$ E\left(x,\dot{x}\right)=\frac{1}{2}{\dot{x}}^{\top}\dot{x}+\Pi (x) $$ can be used to establish global asymptotic stability of the Liénard Equation (6), however, E$$ E $$ is not a strict Lyapunov function in this case, then a variant of such a Lyapunov function V$$ V $$ was proposed in Reference 37 being strict and guaranteeing asymptotic stability of the origin locally. Using properties of homogeneous functions (i.e., …”
Section: Resultsmentioning
confidence: 99%
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“…Let us choose a Lyapunov function for (5) as follows: Vfalse(x,truex˙false)=12truex˙truex˙+normalΠfalse(xfalse)prefix−δtruex˙λprefix−1xtruex˙+εxσprefix−1xtruex˙,$$ V\left(x,\dot{x}\right)=\frac{1}{2}{\dot{x}}^{\top}\dot{x}+\Pi (x)-\delta {\left\Vert \dot{x}\right\Vert}^{\lambda -1}{x}^{\top}\dot{x}+\varepsilon {\left\Vert x\right\Vert}^{\sigma -1}{x}^{\top}\dot{x}, $$ where δ$$ \delta $$ and ε$$ \varepsilon $$ are positive coefficients, λ1$$ \lambda \ge 1 $$, σ1$$ \sigma \ge 1 $$ are powers to be properly selected. Note that the full energy Efalse(x,truex˙false)=12truex˙truex˙+normalΠfalse(xfalse)$$ E\left(x,\dot{x}\right)=\frac{1}{2}{\dot{x}}^{\top}\dot{x}+\Pi (x) $$ can be used to establish global asymptotic stability of the Liénard Equation (6), however, E$$ E $$ is not a strict Lyapunov function in this case, then a variant of such a Lyapunov function V$$ V $$ was proposed in Reference 37 being strict and guaranteeing asymptotic stability of the origin locally. Using properties of homogeneous functions (i.e., …”
Section: Resultsmentioning
confidence: 99%
“…which is asymptotically stable at the origin, [35][36][37] and the remaining terms d(t) + Δ(x t , ̇xt ) are considered as perturbations. For the rest of the proof, all computations are done for the case h > 0, and if h = 0, then the arguments stay unchanged by imposing the respective terms to be zero.…”
Section: General Casementioning
confidence: 99%
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“…which is asymptotically stable at the origin [27], [28], [29], and the remaining terms are considered as perturbations.…”
Section: Resultsmentioning
confidence: 99%
“…ẋ2 + β µ+1 x µ+1 can be used to establish global asymptotic stability of the Liénard equation ( 6), however, E is not a strict Lyapunov function in this case, then V was proposed in [29] being strict and guaranteeing asymptotic stability only locally.…”
Section: Resultsmentioning
confidence: 99%