Abstract:We consider a Boussinesq system of KdV-KdV type introduced by J. Bona, M. Chen and J.-C. Saut as a model for the motion of small amplitude long waves on the surface of an ideal fluid. This system of two equations can describe the propagation of waves in both directions, while the single KdV equation is limited to unidirectional waves. We are concerned here with the exact controllability of the Boussinesq system by using some boundary controls. By reducing the controllability problem to a spectral problem which… Show more
“…Before closing this section, we mention the work [12], in which the boundary controllability problem was addressed for a Boussinesq system of KdV type.…”
Section: Historical Backgroundmentioning
confidence: 99%
“…in Q, u(⋅, 0) = u(⋅, L) = u x (⋅, L) = 0, on (0, T ), v(⋅, 0) = v(⋅, L) = v x (⋅, L) = 0, on (0, T ), u(0, ⋅) = u 0 , v(0, ⋅) = v 0 , on (0, L),(4 12). …”
In this paper, we prove the local null controllability property for a nonlinear coupled system of two Korteweg–de Vries equations posed on a bounded interval and with a source term decaying exponentially on [Formula: see text]. The system was introduced by Gear and Grimshaw to model the interactions of two-dimensional, long, internal gravity waves propagation in a stratified fluid. We address the controllability problem by means of a control supported on an interior open subset of the domain and acting on one equation only. The proof consists mainly on proving the controllability of the linearized system, which is done by getting a Carleman estimate for the adjoint system. While doing the Carleman, we improve the techniques for dealing with the fact that the solutions of dispersive and parabolic equations with a source term in [Formula: see text] have a limited regularity. A local inversion theorem is applied to get the result for the nonlinear system.
“…Before closing this section, we mention the work [12], in which the boundary controllability problem was addressed for a Boussinesq system of KdV type.…”
Section: Historical Backgroundmentioning
confidence: 99%
“…in Q, u(⋅, 0) = u(⋅, L) = u x (⋅, L) = 0, on (0, T ), v(⋅, 0) = v(⋅, L) = v x (⋅, L) = 0, on (0, T ), u(0, ⋅) = u 0 , v(0, ⋅) = v 0 , on (0, L),(4 12). …”
In this paper, we prove the local null controllability property for a nonlinear coupled system of two Korteweg–de Vries equations posed on a bounded interval and with a source term decaying exponentially on [Formula: see text]. The system was introduced by Gear and Grimshaw to model the interactions of two-dimensional, long, internal gravity waves propagation in a stratified fluid. We address the controllability problem by means of a control supported on an interior open subset of the domain and acting on one equation only. The proof consists mainly on proving the controllability of the linearized system, which is done by getting a Carleman estimate for the adjoint system. While doing the Carleman, we improve the techniques for dealing with the fact that the solutions of dispersive and parabolic equations with a source term in [Formula: see text] have a limited regularity. A local inversion theorem is applied to get the result for the nonlinear system.
“…Then, as an application of the newly established exact controllability results, some simple feedback controls are constructed for some particular choice of the parameters, such that the resulting closed-loop systems are exponentially stable. Later on, the stabilization problem was studied in [8,16] for Boussinesq system of KdV-KdV type (b = d = 0) posed on a bounded interval. In any case, depending on the values of its parameters, system (3) couples two equations that may be of KdV-KdV or BBM-BBM types.…”
Section: Decay Of Solutions For a Dissipative Boussinesq System 749mentioning
In this paper we are concerned with a Boussinesq system for smallamplitude long waves arising in nonlinear dispersive media. Considerations will be given for the global well-posedness and the time decay rates of solutions when the model is posed on a periodic domain and a general class of damping operator acts in each equation. By means of spectral analysis and Fourier expansion, we prove that the solutions of the linearized system decay uniformly or not to zero, depending on the parameters of the damping operators. In the uniform decay case, the result is extended for the full system.
“…To prove it, we use the classical approach given by the Riesz representation Theorem to obtain a solution by transposition, see [5,6] for more details. Our analysis on the case of regular data (Theorem 1.1) suggests that is possible to obtain the rapid exponential stabilization for the linear system (5.5) for less regularity of the initial data whenever the linear system is well-posedness in some sense on X 0 .…”
Section: Further Comments and Open Problemsmentioning
confidence: 99%
“…satisfies η(•, T ) = η T and w(•, T ) = w T ? More recently, in [6] (see also [5]), the exact boundary controllability of the linear system Boussinesq of KdV-KdV type was studied. It was discovered that whether the associated linear system is exactly controllable or not depends on the length of the spatial domain.…”
This work deals with the local rapid exponential stabilization for a Boussinesq system of KdV-KdV type introduced by J. Bona, M. Chen and J.-C. Saut. This is a model for the motion of small amplitude long waves on the surface of an ideal fluid. Here, we will consider the Boussinesq system of KdV-KdV type posed on a finite domain, with homogeneous Dirichlet-Neumann boundary controls acting at the right end point of the interval. Our goal is to build suitable integral transformations to get a feedback control law that leads to the stabilization of the system. More precisely, we will prove that the solution of the closed-loop system decays exponentially to zero in the L 2 (0, L)-norm and the decay rate can be tuned to be as large as desired if the initial data is small enough.2010 Mathematics Subject Classification. Primary: 93B05, 93D15, 35Q53.
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