Exponential stability of singularly perturbed systems with mixed impulses (Q2061282)

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scientific article; zbMATH DE number 7443560
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Exponential stability of singularly perturbed systems with mixed impulses
scientific article; zbMATH DE number 7443560

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    Exponential stability of singularly perturbed systems with mixed impulses (English)
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    13 December 2021
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    In this paper, some sufficient conditions have been derived to ensure the global uniform exponential stability of hybrid systems, where the flow dynamics is unstable and exhibits a two-time-scale feature, while the jump dynamics contains both destabilizing and stabilizing impulses simultaneously. The mathematical framework is given by the singular perturbation theory and the system is described as \[ \begin{bmatrix} \dot x(t) \\ \varepsilon\dot z(t) \end{bmatrix} = \begin{bmatrix} A_{11} & A_{12} \\ A_{21} & A_{22} \end{bmatrix} \begin{bmatrix} x(t) \\ z(t) \end{bmatrix},\ t\in [t_k,t_{k+1}), \] \[ \begin{bmatrix} x(t_k) \\ z(t_k) \end{bmatrix} = \begin{bmatrix} D_{11} & D_{12} \\ D_{21} & D_{22} \end{bmatrix} \begin{bmatrix} x(t_k^-) \\ z(t_k^-) \end{bmatrix},\ k\in \mathbb{N}, \] where \(x(t)\in\mathbb{R}^{n_x}\) is the slow state vector, \(z(t)\in\mathbb{R}^{n_z}\) is the fast state vector, \(\varepsilon\) is a small parameter that indicates the degree of the fast and slow dynamics separation. \(A_{ij},\) \(D_{ij},\) \(i = 1, 2,\) \(j = 1,2\) are constant real matrices with appropriate dimensions and the matrix \(A_{22}\) is assumed to be Hurwitz. A new kind of impulse-dependent vector Lyapunov function has been constructed to explore the positive effect of the stabilizing impulse and describe the relationship between two consecutive impulses.
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    singularly perturbed system
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    mixed impulse
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    exponential stability
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    vector Lyapunov function
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