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Instability in the critical case of pair of pure imaginary roots for a class of systems with aftereffect
Institution:1. Guangzhou Institute of Energy Conversion, Chinese Academy of Sciences (CAS), Guangzhou, 510640, China;2. School of Engineering Science, University of Science and Technology of China, Hefei, 230026, China;3. Guangdong Provincial Key Laboratory of New and Renewable Energy Research and Development, Guangzhou, 510640, China;4. Faculty of Materials and Manufacturing, Beijing University of Technology, Beijing, 100124, China;1. Toxoplasmosis Research Center, Mazandaran University of Medical Sciences, Sari, Iran;2. Department of Parasitology and Mycology, Sari Medical School, Mazandaran University of Medical Sciences, Sari, Iran;3. Infectious and Tropical Diseases Research Center, Tabriz University of Medical Sciences, Tabriz, Iran;1. National Electronics and Computer Technology Center (NECTEC), Pathum Thani, Thailand;2. Department of Industrial & Systems Engineering, Rutgers University, Piscataway, NJ, USA;3. Department of Computer Engineering, King Mongkut''s University of Technology Thonburi, Bangkok, Thailand
Abstract:The stability of a system described by Volterra integrodifferential equations is investigated in the critical case when the characteristic equation has a pair of pure imaginery roots. Conditions for instability, analogous to the well-known conditions from the theory of differential equations 1], are derived. (A similar result was established previously in 2] for integrodifferential equations of simpler structure with integral kernels of exponential-polynomial type). For the proof, several manipulations are used to simplify the original equation and, in particular, to reduce the linearized equation to the form of a differential equation with constant diagonal matrix. (An analogous approach was used to analyse instability for Volterra integrodifferential equations in the critical case of zero root in 3, 4]). As an example, the sign of the Lyapunov constant in the problem of the rotational motion of a rigid body with viscoelastic supports is calculated.
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