Controlling Chaos to a Class of PDES by Applying Invariant Manifold and Structure Stability Theory

In this paper, we are concerned with the chaotic behavior of a class of control systems described by partial differential equations. By means of finite dimensional output feedback control, it is shown that the flow on the global attractor is topologically equivalent to that of a finite dimensional difference system. In addition, an example is given to illustrate that the chaotic behavior of the flow on the global attractor can be determined by computing the Lyapunov exponent of an associated finite dimensional difference system.

[1]  Daniel B. Henry,et al.  Some infinite-dimensional Morse-Smale systems defined by parabolic partial differential equations , 1985 .

[2]  H. Shibata Lyapunov exponent of partial differential equation , 1999 .

[3]  Pattern dynamics and spatiotemporal chaos in the conserved Zakharov equations , 2000 .

[4]  N. Kunimatsu,et al.  An application of inertial manifold theory to boundary stabilization of semilinear diffusion systems , 1995 .

[5]  On the bifurcation phenomena in truncations of the 2D Navier-Stokes equations , 1995 .

[6]  K. Lu Structural Stability for Scalar Parabolic Equations , 1994 .

[7]  Y. Li Smale Horseshoes and Symbolic Dynamics in Perturbed Nonlinear Schrödinger Equations , 1999 .

[8]  Ioannis G. Kevrekidis,et al.  Numerical bifurcation and stability analysis of solitary pulses in an excitable reaction—diffusion medium , 1999 .

[9]  Stephen Wiggins,et al.  Homoclinic orbits and chaos in discretized perturbed NLS systems: Part II. Symbolic dynamics , 1997 .

[10]  Markus Bär,et al.  Pulse bifurcation and transition to spatiotemporal chaos in an excitable reaction-diffusion model , 1997 .

[11]  Spatiotemporal chaos in spatially extended systems , 2001 .

[12]  Hildebrando M. Rodrigues,et al.  Upper Semicontinuity of Attractors and Synchronization , 1998 .

[13]  Giorgio Fusco,et al.  Jacobi matrices and transversality , 1987, Proceedings of the Royal Society of Edinburgh: Section A Mathematics.

[14]  R. Russell,et al.  On the Compuation of Lyapunov Exponents for Continuous Dynamical Systems , 1997 .

[15]  B. Buti Control of chaos in dusty plasmas , 1997 .

[16]  A. Brandenburg,et al.  Chaos in Accretion Disk Dynamos , 1995 .

[17]  S. Wiggins,et al.  Homoclinic Orbits in a Four Dimensional Model of a Perturbed NLS Equation: A Geometric Singular Perturbation Study , 1996 .

[18]  D. McLaughlin,et al.  Homoclinic orbits and chaos in discretized perturbed NLS systems: Part I. Homoclinic orbits , 1997 .

[19]  P. Parmananda,et al.  SYNCHRONIZATION OF SPATIOTEMPORAL CHEMICAL CHAOS USING RANDOM SIGNALS , 1998 .

[20]  G. Kovačič Singular perturbation theory for homoclinic orbits in a class of near-integrable dissipative systems , 1995 .

[21]  G. Kovačič,et al.  Orbits homoclinic to resonances, with an application to chaos in a model of the forced and damped sine-Gordon equation , 1992 .

[22]  H. Lai,et al.  Double-mode modeling of chaotic and bifurcation dynamics for a simply supported rectangular plate in large deflection , 2002 .

[23]  Inertial Manifolds and Stabilization of Semilinear Distributed Parameter Systems , 1993 .

[24]  Alexandre N. Carvalho,et al.  The Dynamics of a One-Dimensional Parabolic Problem versus the Dynamics of Its Discretization , 2000 .

[25]  Aranson,et al.  Controlling spatiotemporal chaos. , 1994, Physical review letters.

[26]  Quantitative characterization of spatiotemporal patterns II , 1998 .

[27]  Sergio Albeverio,et al.  Spatial chaos in a fourth-order nonlinear parabolic equation , 2001 .

[28]  H. Lai,et al.  Chaotic and bifurcation dynamics for a simply supported rectangular plate of thermo-mechanical coupling in large deflection , 2002 .

[29]  Inertial Manifolds and Stabilization in Nonlinear Elastic Systems with Structural Damping , 1993 .

[30]  Sze-Bi Hsu,et al.  Snapback repellers as a cause of chaotic vibration of the wave equation with a van der Pol boundary condition and energy injection at the middle of the span , 1998 .