1999
DOI: 10.1016/s0764-4442(99)80434-0
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Stabilisation frontière de problèmes de Ventcel

Abstract: Abstract. The problem of boundary stabilization for the isotropic linear elastodynamic system and the wave equation with Ventcel's conditions are considered (see [12]). The boundary observability and the exact controllability were etablished in [11]. We prove here the enegy decay to zero for the elastodynamic system with stationary Ventcel's conditions by introducing a nonlinear boundary feedback. We also give a boundary feedback leading to arbitrarily large energy decay rates for the elastodynamic system with… Show more

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Cited by 10 publications
(11 citation statements)
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“…4 The study of some mathematical and numerical aspects of such problems were given in Lemrabet 3 and Goldstein. 5 For a detailed survey on Wentzell boundary conditions, we refer the reader to the previous studies [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] and the references therein, and the list is not exhaustive.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…4 The study of some mathematical and numerical aspects of such problems were given in Lemrabet 3 and Goldstein. 5 For a detailed survey on Wentzell boundary conditions, we refer the reader to the previous studies [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] and the references therein, and the list is not exhaustive.…”
Section: Introductionmentioning
confidence: 99%
“…The issue of stability of solutions of the Wentzell problems has attracted a great deal of attention in the last 3 decades. To this end, see, for instance, previous works 4, [7][8][9]14,15,18,19 and the references therein. In Heminna, 14 the author showed that the natural feedback is not sufficient to guarantee the exponential decay of the energy ((t)) in the case of the wave equation with Wentzell conditions.…”
Section: Introductionmentioning
confidence: 99%
“…As mentioned before, A. Heminna has shown in [7,8] that the feedback law on Γ 1 is actually not sufficient to guarantee the exponential decay of the energy even if the subset Γ 1 satisfy the control geometric condition. More precisely the author showed that if Γ 1 = {(1, y) : 0 < y < 1} ∪ {(x, 1) : 0 < x < 1} then the operator A associated with problem (2.1) has eigenvalues that tend to the imaginary axis.…”
Section: The Problemmentioning
confidence: 97%
“…Ventcel boundary conditions are characterized by the presence of tangential differential operators of the same order than the interior operator. Such boundary conditions are usually justified by asymptotic methods and appear in mechanics [13], in diffusion processes [12,21] or wave phenomena [2,[7][8][9]14].…”
Section: Introductionmentioning
confidence: 99%
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