2019
DOI: 10.1016/j.sysconle.2019.104529
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Finite-time internal stabilization of a linear 1-D transport equation

Abstract: We consider a 1-D linear transport equation on the interval (0, L), with an internal scalar control. We prove that if the system is controllable in a periodic Sobolev space of order greater than 1, then the system can be stabilized in finite time, and we give an explicit feedback law.

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Cited by 25 publications
(18 citation statements)
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References 36 publications
(44 reference statements)
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“…There are mainly two ways to prove the existence of the transformation, either by direct methods [18,19] or, more commonly, by proving the existence of a Riesz basis. For the latter, we again distinguish two cases: either the Riesz basis is deduced directly by an isomorphism applied on an eigenbasis [17,50,51] or the existence of a Riesz basis follows by controllability assumptions and sufficient growth of the eigenvalues of the spatial operator allowing in particular to prove that the family is quadratically close to the eigenfunctions [16,20,21,27] (see Section 2.2 and Section 4 for a definition).…”
Section: Related Results: the Heat Equation And The Backstepping Methodsmentioning
confidence: 99%
“…There are mainly two ways to prove the existence of the transformation, either by direct methods [18,19] or, more commonly, by proving the existence of a Riesz basis. For the latter, we again distinguish two cases: either the Riesz basis is deduced directly by an isomorphism applied on an eigenbasis [17,50,51] or the existence of a Riesz basis follows by controllability assumptions and sufficient growth of the eigenvalues of the spatial operator allowing in particular to prove that the family is quadratically close to the eigenfunctions [16,20,21,27] (see Section 2.2 and Section 4 for a definition).…”
Section: Related Results: the Heat Equation And The Backstepping Methodsmentioning
confidence: 99%
“…However the equation above is actually purely formal, and the "right way" to formulate it is the weak form in (310), which is not surprising, as, according to Corollary 5.1, T I ν is not defined and thus (311) has no real mathematical meaning. This is already the case for transport equations ( [73,74]).…”
Section: Finding a Suitable Candidate: The Operator Equalitymentioning
confidence: 70%
“…Also, several results (e.g. [16]) were obtained using a backstepping approach, a very powerful method based on a Volterra transformation, developed mainly for PDE in [24], and generalized recently with a Fredholm transformation for hyperbolic systems [14,34,35]. One may look at [22] for a more detailed survey about this method and its use for the Saint-Venant equations.…”
Section: Introductionmentioning
confidence: 99%