“…As one can note, it has the same form of the derivative of the boundary datum and hence it vanishes for long times. In Figure 14 we present a section of the solution u(x, y, t) of the problem (23)- (25), in the same point x = 1 2 , for t ∈[0, 10]: as one can observe, the wave travelling away from the boundary assumes the same structure of the Dirichlet boundary datum but with diminishing intensity. Figure 15 shows the time-dependent behavior of the solution u(x, t) outside .…”
Section: Numerical Resultsmentioning
confidence: 97%
“…As we have seen for 1D problems, we can consider the single-layer representation of the solution of (23)- (25):…”
Section: Dirichlet Problem and Its Energetic Weak Formulationmentioning
International audienceIn this paper we consider Dirichlet or Neumann wave propagation problems reformulated in terms of boundary integral equations with retarded potential. Starting from a natural energy identity, a space–time weak formulation for 1D integral problems is briefly introduced, and continuity and coerciveness properties of the related bilinear form are proved. Then, a theoretical analysis of an extension of the introduced formulation for 2D problems is proposed, pointing out the novelty with respect to existing literature results. At last, various numerical simulations will be presented and discussed, showing unconditional stability of the space–time Galerkin boundary element method applied to the energetic weak problem
“…As one can note, it has the same form of the derivative of the boundary datum and hence it vanishes for long times. In Figure 14 we present a section of the solution u(x, y, t) of the problem (23)- (25), in the same point x = 1 2 , for t ∈[0, 10]: as one can observe, the wave travelling away from the boundary assumes the same structure of the Dirichlet boundary datum but with diminishing intensity. Figure 15 shows the time-dependent behavior of the solution u(x, t) outside .…”
Section: Numerical Resultsmentioning
confidence: 97%
“…As we have seen for 1D problems, we can consider the single-layer representation of the solution of (23)- (25):…”
Section: Dirichlet Problem and Its Energetic Weak Formulationmentioning
International audienceIn this paper we consider Dirichlet or Neumann wave propagation problems reformulated in terms of boundary integral equations with retarded potential. Starting from a natural energy identity, a space–time weak formulation for 1D integral problems is briefly introduced, and continuity and coerciveness properties of the related bilinear form are proved. Then, a theoretical analysis of an extension of the introduced formulation for 2D problems is proposed, pointing out the novelty with respect to existing literature results. At last, various numerical simulations will be presented and discussed, showing unconditional stability of the space–time Galerkin boundary element method applied to the energetic weak problem
“…To simplify the notation, we do not point it out. The above theorem was proved in [8], [22]; see also [2], [3], [9], [11], [12], [13], [14], [15], [16], [17], [20], [21] for a more complete treatment.…”
Abstract. The paper deals with recovering band-and energy-limited signals from a finite set of perturbed inner products involving the prolate spheroidal wavefunctions. The measurement noise (bounded by δ) and jitter meant as perturbation of the ends of the integration interval (bounded by γ) are considered. The upper and lower bounds on the radius of information are established. We show how the error of the best algorithms depends on γ and δ. We prove that jitter causes error of order Ω 3 2 γ, where [−Ω, Ω] is a bandwidth, which is similar to the error caused by jitter in the case of recovering signals from samples.
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