“…The time integrals appearing in the definition of the single and double layer operators (see (3), (4)) are discretized by means of the above mentioned second order Lubich convolution quadrature formula (see [14]). We obtain:…”
Section: Approximation In Timementioning
confidence: 99%
“…Furthermore, they are generally used to determine the problem solution at chosen points. Only in the last few years (see [13], [2], [14], [6]), a BIE for the classical wave equation has been used to define a Non Reflecting Boundary Condition (NRBC) on a chosen artificial boundary, surrounding the computational domain. Its discretization is then coupled with that of the domain of interest by means of finite elements or finite differences.…”
Section: Introductionmentioning
confidence: 99%
“…To solve problem (1) we will consider the following single-double layer BIE (see [14]): 1 2 u e (x, t) − (V∂ n u e )(x, t) + (Ku e )(x, t) = I u 0 (x, t) + The last expressions in (3) and (4) have been obtained by interchanging (see [15]) the time and space integrals in the corresponding representations, and using the wave equation fundamental solution expression…”
Section: Introductionmentioning
confidence: 99%
“…Very recently, in [14] (see also [6]), for the solution of (1), we have proposed to use (2) as a global Non Reflecting Boundary Condition, to be imposed on a chosen artificial boundary B delimiting the domain of interest Ω. This NRBC is interpreted as a relationship that the problem solution and its normal derivative must satisfy on B, to avoid spurious wave reflections.…”
On the discretization and application of two space-time boundary integral equations for 3D wave propagation problems in unbounded domains / Falletta, Silvia; Monegato, Giovanni; Scuderi, Letizia.-In: APPLIED NUMERICAL MATHEMATICS.
“…The time integrals appearing in the definition of the single and double layer operators (see (3), (4)) are discretized by means of the above mentioned second order Lubich convolution quadrature formula (see [14]). We obtain:…”
Section: Approximation In Timementioning
confidence: 99%
“…Furthermore, they are generally used to determine the problem solution at chosen points. Only in the last few years (see [13], [2], [14], [6]), a BIE for the classical wave equation has been used to define a Non Reflecting Boundary Condition (NRBC) on a chosen artificial boundary, surrounding the computational domain. Its discretization is then coupled with that of the domain of interest by means of finite elements or finite differences.…”
Section: Introductionmentioning
confidence: 99%
“…To solve problem (1) we will consider the following single-double layer BIE (see [14]): 1 2 u e (x, t) − (V∂ n u e )(x, t) + (Ku e )(x, t) = I u 0 (x, t) + The last expressions in (3) and (4) have been obtained by interchanging (see [15]) the time and space integrals in the corresponding representations, and using the wave equation fundamental solution expression…”
Section: Introductionmentioning
confidence: 99%
“…Very recently, in [14] (see also [6]), for the solution of (1), we have proposed to use (2) as a global Non Reflecting Boundary Condition, to be imposed on a chosen artificial boundary B delimiting the domain of interest Ω. This NRBC is interpreted as a relationship that the problem solution and its normal derivative must satisfy on B, to avoid spurious wave reflections.…”
On the discretization and application of two space-time boundary integral equations for 3D wave propagation problems in unbounded domains / Falletta, Silvia; Monegato, Giovanni; Scuderi, Letizia.-In: APPLIED NUMERICAL MATHEMATICS.
“…The papers [1,9] deal with four-field formulations (two fields in the interior domain and two on the boundary) and aim at coupling an explicit interior time-stepping method with the retarded boundary integral equations on the boundary, differing in the use of Galerkin-in-time or CQ for the equations on the boundary. The papers [15,13,14] contain successful computational studies of one-equation couplings, although a theoretical understanding of their stability is still missing. A preliminary semidiscrete stability analysis in the Laplace domain of the coupling method we will study here appears in [24].…”
We study a symmetric BEM-FEM coupling scheme for the scattering of transient acoustic waves by bounded inhomogeneous anisotropic obstacles in a homogeneous field. An incident wave in free space interacts with the obstacles and produces a combination of transmission and scattering. The transmitted part of the wave is discretized in space by finite elements while the scattered wave is reduced to two fields defined on the boundary of the obstacles and is discretized in space with boundary elements. We choose a coupling formulation that leads to a symmetric system of integro-differential equations. The retarded boundary integral equations are discretized in time by Convolution Quadrature, and the interior field is discretized in time with the trapezoidal rule. We show that the scattering problem generates a C 0 group of isometries in a Hilbert space, and use associated estimates to derive stability and convergence results. We provide numerical experiments and simulations to validate our results and demonstrate the flexibility of the method.
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