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handle: 11588/168671 , 11572/36269
The authors consider the equation \[ \dot x = f(t,x),\quad x(t_0) = x_0,\tag{1} \] where \(f\in C(\mathbb{R}^+\times D,\mathbb{R}^s)\) is locally Lipschitzian in \(x\), \(f(t,0)\equiv 0\), \(D\subset \mathbb{R}^s\), and the perturbed equation \[ \dot x = g(t,x,\lambda),\quad x(t_0) = x_0,\tag{2} \] where \(g: \mathbb{R}^+\times D\times\Lambda\to \mathbb{R}^s\) be a mapping such that: (i) for each \(\lambda\in\Lambda\) the function \(g(\cdot,\cdot,\lambda)\) is locally Lipschitzian in \(x\), and (ii) \(g(\cdot,\cdot,\lambda) = f\) if and only if \(\lambda = 0\). Let \({\mathcal U} = \{g(\cdot,\cdot,\lambda)-f: \lambda\in\Lambda\}\) be the set of perturbations corresponding to \(\Lambda\) and denote by \({\mathcal U}^*\) the set \({\mathcal U}-\{0\}\). Let \(g(t,0,\lambda) = 0\) and (2) admits the solution \(x(t)=0\). The solution \(x(t)=0\) to the unperturbed equation (1) is said to be \({\mathcal U}^*\)-secularly stable if \(x(t)\equiv 0\) is a uniformly stable solution to (2) for any \(\lambda \in\Lambda-\{0\}\). The theorems on the secular stability are proved and applied to holonomic systems.
differential equations; stability; holonomic systems; cyclic coordinates; dissipative perturbations, Stability for nonlinear problems in mechanics, differential equations, dissipative perturbations, stability, cyclic coordinates, Stability problems for infinite-dimensional dissipative dynamical systems, Structural stability and analogous concepts of solutions to ordinary differential equations, Stability problems for problems in Hamiltonian and Lagrangian mechanics, Holonomic systems related to the dynamics of a system of particles, holonomic systems
differential equations; stability; holonomic systems; cyclic coordinates; dissipative perturbations, Stability for nonlinear problems in mechanics, differential equations, dissipative perturbations, stability, cyclic coordinates, Stability problems for infinite-dimensional dissipative dynamical systems, Structural stability and analogous concepts of solutions to ordinary differential equations, Stability problems for problems in Hamiltonian and Lagrangian mechanics, Holonomic systems related to the dynamics of a system of particles, holonomic systems
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