2021
DOI: 10.1051/cocv/2021067
|View full text |Cite
|
Sign up to set email alerts
|

One-dimensional wave equation with set-valued boundary damping: well-posedness, asymptotic stability, and decay rates

Abstract: This paper is concerned with the analysis of a 1D wave equation $z_{tt}-z_{xx}=0$ on $[0,1]$ with a Dirichlet condition at $x=0$ and a damping acting at $x=1$ of the form  $(z_t(t,1),-z_x(t,1))\in\Sigma$ for $t\geq 0$, where $\Sigma$ is a given subset of $\mathbb R^2$. The study is performed within an $L^p$ functional framework, $p\in [1, +\infty]$. We determine conditions on $\Sigma$ ensuring existence and uniqueness of solutions of that wave equation,  its strong stability and uniform global asymptotic stabi… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
3
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
4
1

Relationship

0
5

Authors

Journals

citations
Cited by 9 publications
(3 citation statements)
references
References 24 publications
0
3
0
Order By: Relevance
“…Here, using the terminology of [21], the feedback is allowed to be weak, i.e., g(s)/s can go to 0 as |s| goes to infinity, as it is the case when g represents a saturation mapping; then, loss of uniformity is to be expected. More precisely, coming back to the Neumann problem, the one-dimensional version of (1.6) with g given by (1.7) is known to possess weak solutions that decay to zero (in the natural energy space H 1 (Ω) × L 2 (Ω)) slower than any exponential or polynomial, whereas strong solutions decay exponentially to zero but in a non-uniform way -see [21,Theorem 4.1] or also [1,Theorem 4.33]. Proving a similar result in our Dirichlet case would be interesting.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Here, using the terminology of [21], the feedback is allowed to be weak, i.e., g(s)/s can go to 0 as |s| goes to infinity, as it is the case when g represents a saturation mapping; then, loss of uniformity is to be expected. More precisely, coming back to the Neumann problem, the one-dimensional version of (1.6) with g given by (1.7) is known to possess weak solutions that decay to zero (in the natural energy space H 1 (Ω) × L 2 (Ω)) slower than any exponential or polynomial, whereas strong solutions decay exponentially to zero but in a non-uniform way -see [21,Theorem 4.1] or also [1,Theorem 4.33]. Proving a similar result in our Dirichlet case would be interesting.…”
Section: Discussionmentioning
confidence: 99%
“…In the one-dimensional settings, arguments based on Riemann invariants are available, and the decay of the energy can be analyzed via appropriate iterated sequences. See for instance [1], where g is allowed to be a multivalued monotone mapping, or [21], where it is proved, in particular, that exponential or polynomial uniform decay cannot be achieved when g represents a pointwise saturation mapping -see also [22] or [16] for a stability analysis in the saturated case.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, most of the existing works give their stability results in the Hilbertian space L 2 . Let us mention however some recent works in that direction: [12], [3] or [11]. We also emphasize on the fact that our approach is adjustable to more general SMC methods such as adaptive approaches.…”
Section: Introductionmentioning
confidence: 99%