doi:10.1016/j.automatica.2007.05.012
Copyright © 2007 Elsevier Ltd All rights reserved.
Output-feedback stabilization of an unstable wave equation
aDepartment of Mechanical and Aerospace Engineering, University of California at San Diego, 9500 Gilman Drive, La Jolla, CA 92093-0411, USA
bInstitute of Systems Science, Academy of Mathematics and Systems Science, Academia Sinica, Beijing 100080, PR China
cSchool of Computational and Applied Mathematics, University of the Witwatersrand, Wits 2050, Johannesburg, South Africa
dDepartment of Mathematics, University of Texas - Pan American, 1201 W. University Drive, Edinburg, TX 78541-2999, USA
Received 7 September 2006;
revised 11 April 2007;
accepted 11 May 2007.
Available online 28 August 2007.
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Abstract
We consider the problem of stabilization of a one-dimensional wave equation that contains instability at its free end and control on the opposite end. In contrast to classical collocated “boundary damper” feedbacks for the neutrally stable wave equations with one end satisfying a homogeneous boundary condition, the controllers and the associated observers designed in the paper are more complex due to the open-loop instability of the plant. The controller and observer gains are designed using the method of “backstepping,” which results in explicit formulae for the gain functions. We prove exponential stability and the existence and uniqueness of classical solutions for the closed-loop system. We also derive the explicit compensators in frequency domain. The results are illustrated with simulations.
Keywords: Distributed parameter systems; Wave equation; Backstepping; Stabilization; Boundary control
Fig. 1. Two problem formulations for boundary control of a stable string pinned on one end: top—classical formulation with the actuation/sensing collocated on the right end (Neuman/force actuation and Dirichlet/displacement sensing). Bottom (Guo & Xu, 2007)—Neumann actuation on the right end and Neumann sensing on the left (pinned) end.
Fig. 2. Two problem formulations for boundary control of an unstable string with a destabilizing force (boundary condition) on the free end: top (Sections 2–5)—Dirichlet actuation on the right end, Dirichlet sensing on the left end. Bottom (Section 6)—collocated actuation/sensing on the right end (Neumann/force actuation and Dirichlet/displacement sensing).
Fig. 3. Bode plots of the plant (dashed) and the compensator (solid) for the non-collocated design.
Fig. 4. String response w(x,t). Uncontrolled case, zero Dirichlet boundary condition at x=1.
Fig. 5. Observer error
in the uncontrolled case.
Fig. 6. String response w(x,t) with observer-based control applied at x=1.
Fig. 7. Time trace of control u(t).
Fig. 8. String response w(x,t) with reduced order (N=6) observer-based control applied at x=1.
Fig. 9. String response w(x,t) with q=1 in the observer mismatching the value q=1.1 in the plant.
Fig. 10. Closed-loop poles: ×—nominal plant and compensator (q=1),
—plant with q=1.1, but compensator is designed for q=1.