Instability in the critical case of a pair of pure imaginary roots for a class of systems with aftereffect (Q2714639)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Instability in the critical case of a pair of pure imaginary roots for a class of systems with aftereffect |
scientific article; zbMATH DE number 1607056
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Instability in the critical case of a pair of pure imaginary roots for a class of systems with aftereffect |
scientific article; zbMATH DE number 1607056 |
Statements
20 June 2001
0 references
integro-differential system
0 references
couple of pure imaginary roots
0 references
Instability in the critical case of a pair of pure imaginary roots for a class of systems with aftereffect (English)
0 references
The system of integro-differential equations NEWLINE\[NEWLINE \frac{dx}{dt} = Ax +\int_0^t K(t-s)x(s) ds + F(x,\widetilde{y},t),\quad x\in \mathbb{R}^n,\quad \widetilde{y}\in \mathbb{R}^m,\tag{1} NEWLINE\]NEWLINE is considered, where \(A\) is a constant \(n\times n\)-matrix, \( K(t)\in C(\mathbb{R}_+,\mathbb{R}^{n\times n}) \) and \( \|K(t)\|\leq C \exp(-\beta t)\), \( C\), \(\beta=\text{const}>0\). It is assumed that the characteristic equation corresponding to (1) has a couple of pure imaginary roots. Instability conditions are established for the solutions to system (1). The sign of the Lyapunov constant is determined in the problem on rotating motion of a solid with visco-elastic supports.
0 references