“…Since P h1,h2 y h1,h2 belongs to H 1 0 (Ω h1,h2 ) ⊂ H 1 0 (B), the limitỹ(t) belongs to H 1 0 (B). Furthermore, since ∂Ω is Lipschitz by assumption and also ∂Ω h1,h2 by construction, it possess the so-called -cone property, introduced in [4]. This implies that the bounded sequence (Ω h1,h2 ) h1,h2 defined, for each h 1 , h 2 fixed, as the largest domain included in Ω and union of cell B j,k converges towards Ω with respect to the complementary-Hausdorff topology (see [20]).…”
Section: Step 3 Property Ofỹ(t) For All T ≥mentioning
confidence: 97%
“…The objects corresponding to this example are summarized on (3,1), (3,5), (7,3), (9, 0), (9, 1), (9, 2), (9, 4), (9, 5)}, (3,5), (4,5), (7,3), (8,3), (9,3), (1,6), (2,6), (5,6), (6,6), (7,6), (8,6)}.…”
Abstract. This work is devoted to the analysis of a viscous finite-difference space semi-discretization of a locally damped wave equation in a regular 2-D domain. The damping term is supported in a suitable subset of the domain, so that the energy of solutions of the damped continuous wave equation decays exponentially to zero as time goes to infinity. Using discrete multiplier techniques, we prove that adding a suitable vanishing numerical viscosity term leads to a uniform (with respect to the mesh size) exponential decay of the energy for the solutions of the numerical scheme. The numerical viscosity term damps out the high frequency numerical spurious oscillations while the convergence of the scheme towards the original damped wave equation is kept, which guarantees that the low frequencies are damped correctly. Numerical experiments are presented and confirm these theoretical results. These results extend those by Tcheugoué-Tébou and Zuazua [Numer. Math. 95, 563-598 (2003)] where the 1-D case was addressed as well the square domain in 2-D. The methods and results in this paper extend to smooth domains in any space dimension.Mathematics Subject Classification. 65M06.
“…Since P h1,h2 y h1,h2 belongs to H 1 0 (Ω h1,h2 ) ⊂ H 1 0 (B), the limitỹ(t) belongs to H 1 0 (B). Furthermore, since ∂Ω is Lipschitz by assumption and also ∂Ω h1,h2 by construction, it possess the so-called -cone property, introduced in [4]. This implies that the bounded sequence (Ω h1,h2 ) h1,h2 defined, for each h 1 , h 2 fixed, as the largest domain included in Ω and union of cell B j,k converges towards Ω with respect to the complementary-Hausdorff topology (see [20]).…”
Section: Step 3 Property Ofỹ(t) For All T ≥mentioning
confidence: 97%
“…The objects corresponding to this example are summarized on (3,1), (3,5), (7,3), (9, 0), (9, 1), (9, 2), (9, 4), (9, 5)}, (3,5), (4,5), (7,3), (8,3), (9,3), (1,6), (2,6), (5,6), (6,6), (7,6), (8,6)}.…”
Abstract. This work is devoted to the analysis of a viscous finite-difference space semi-discretization of a locally damped wave equation in a regular 2-D domain. The damping term is supported in a suitable subset of the domain, so that the energy of solutions of the damped continuous wave equation decays exponentially to zero as time goes to infinity. Using discrete multiplier techniques, we prove that adding a suitable vanishing numerical viscosity term leads to a uniform (with respect to the mesh size) exponential decay of the energy for the solutions of the numerical scheme. The numerical viscosity term damps out the high frequency numerical spurious oscillations while the convergence of the scheme towards the original damped wave equation is kept, which guarantees that the low frequencies are damped correctly. Numerical experiments are presented and confirm these theoretical results. These results extend those by Tcheugoué-Tébou and Zuazua [Numer. Math. 95, 563-598 (2003)] where the 1-D case was addressed as well the square domain in 2-D. The methods and results in this paper extend to smooth domains in any space dimension.Mathematics Subject Classification. 65M06.
“…Let us recall some classical properties of the Hausdorff convergence, for the proofs we refer to [8,11], or [3]. …”
Section: Continuity With Respect To the Domainmentioning
confidence: 99%
“…Moreover, we know (cf. [8] or [3]) that we are always able to choose the sequence of associated cone directions ξ Xn in order that they converge to ξ X . Therefore, for n large enough, the boundary of ω n in a neighbourhood of X n can be written as a graph of a function ψ n (L + 1)-Lipschitzian in some local coordinate system R X associated to the point X with vertical vector ξ X (see (15)).…”
Section: If ω N Is a Sequence Of Sets In The Class C Which Goes To Inmentioning
confidence: 99%
“…This class can also be described as sets with the ε-cone property, and it has been introduced by Chenais in her important work, see [3,4]. In Section 1.2, we recall the definition of the ε-cone property.…”
Abstract. In this paper, we are interested in finding the optimal shape of a magnet. The criterion to maximize is the jump of the electromagnetic field between two different configurations. We prove existence of an optimal shape into a natural class of domains. We introduce a quasi-Newton type algorithm which moves the boundary. This method is very efficient to improve an initial shape. We give some numerical results.Mathematics Subject Classification. 49J20, 49Q10, 65K10, 78A30.
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