Implicit one-dimensional discrete maps and their connection with existence problem of chaotic dynamics in 3-D systems of differential equations (Q440795)
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: Implicit one-dimensional discrete maps and their connection with existence problem of chaotic dynamics in 3-D systems of differential equations |
scientific article; zbMATH DE number 6068324
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Implicit one-dimensional discrete maps and their connection with existence problem of chaotic dynamics in 3-D systems of differential equations |
scientific article; zbMATH DE number 6068324 |
Statements
Implicit one-dimensional discrete maps and their connection with existence problem of chaotic dynamics in 3-D systems of differential equations (English)
0 references
19 August 2012
0 references
implicit one-dimensional discrete map
0 references
ordinary autonomous differential equations system
0 references
limit cycle
0 references
chaotic dynamics
0 references
0 references
0 references
0 references
0 references
0.90515465
0 references
0.88198453
0 references
0 references
0.86617804
0 references
0.8644065
0 references
0.8622014
0 references
0.86186117
0 references
0.86074907
0 references
0.85924596
0 references
The present paper is a continuation of the work [Appl. Math. Comput. 218, No. 8, 4546--4566 (2011; Zbl 1247.34069)].NEWLINENEWLINEIn this paper, the following autonomous chaotic system is considered NEWLINE\[NEWLINE\begin{cases} \dot{x}(t)= a_1 x(t) + a_{11} y^2(t) + a_{12}y(t) z(t) + a_{22} z^2(t),\\ \dot{x}(t)= b_1 y(t)+ c_1 z(t) + bx(t)y (t),\\ \dot{z}(t)= c_1(t)+ b_1 z(t) + cx(t)z(t), \end{cases}NEWLINE\]NEWLINE NEWLINEwhere \(a_1\), \(a_{11}\), \(a_{12}\),\dots, \(c_1\), \(b_1\), \(c\) are coefficients. Each equation of the system has a quadratic term.NEWLINENEWLINEFor some values of the coefficients, the system can exhibit Lorenz-type attractors. Basic properties of the dynamical system have been analyzed by the means of Lyapunov exponents and Poincaré map. This analysis verifies the existence of chaotic dynamics in the system. The author gives a detailed investigation of the characteristics of this system.
0 references