On stability of zero solution of an essentially nonlinear second-order differential equation
Autor: | V. A. Pliss, Yu. N. Bibikov, N. V. Trushina |
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Rok vydání: | 2017 |
Předmět: |
Lyapunov function
Polynomial Differential equation General Mathematics 010102 general mathematics Mathematical analysis 02 engineering and technology 01 natural sciences Periodic function symbols.namesake Nonlinear system 020303 mechanical engineering & transports 0203 mechanical engineering Dissipative system symbols Restoring force 0101 mathematics Constant (mathematics) Mathematics |
Zdroj: | Vestnik St. Petersburg University, Mathematics. 50:235-241 |
ISSN: | 1934-7855 1063-4541 |
DOI: | 10.3103/s1063454117030062 |
Popis: | Small periodic (with respect to time) perturbations of an essentially nonlinear differential equation of the second order are studied. It is supposed that the restoring force of the unperturbed equation contains both a conservative and a dissipative part. It is also supposed that all solutions of the unperturbed equation are periodic. Thus, the unperturbed equation is an oscillator. The peculiarity of the considered problem is that the frequency of oscillations is an infinitely small function of the amplitude. The stability problem for the zero solution is considered. Lyapunov investigated the case of autonomous perturbations. He showed that the asymptotic stability or the instability depends on the sign of a certain constant and presented a method to compute it. Liapunov’s approach cannot be applied to nonautonomous perturbations (in particular, to periodic ones), because it is based on the possibility to exclude the time variable from the system. Modifying Lyapunov’s method, the following results were obtained. “Action–angle” variables are introduced. A polynomial transformation of the action variable, providing a possibility to compute Lyapunov’s constant, is presented. In the general case, the structure of the polynomial transformation is studied. It turns out that the “length” of the polynomial is a periodic function of the exponent of the conservative part of the restoring force in the unperturbed equation. The least period is equal to four. |
Databáze: | OpenAIRE |
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