2019
DOI: 10.1016/j.jsv.2018.08.059
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Numerical modelling of sound propagation in rooms bounded by walls with rectangular-shaped irregularities and frequency-dependent impedance

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Cited by 12 publications
(8 citation statements)
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“…A wide variety of numerical methods are available for timedomain simulations: finite-difference time-domain (FDTD) (Sakamoto, 2007;Kowalczyk and van Walstijn, 2008;Sakamoto et al, 2008;Kowalczyk and van Walstijn, 2011;Hamilton and Bilbao, 2017;Toyoda and Eto, 2019;Cingolani et al, 2021;Toyoda and Sakayoshi, 2021) or finite-volume timedomain (FVTD) methods (Bilbao, 2013;Bilbao et al, 2016), time-domain BEM (TD-BEM) (Hargreaves and Cox, 2008), time-domain FEM (TD-FEM) (Okuzono et al, 2019;Yoshida et al, 2022), time-domain discontinuous Galerkin FEM (DG-FEM) (Simonaho et al, 2012;Wang et al, 2019;Wang and Hornikx, 2020;Pind et al, 2021), time-domain spectral element method (TD-SEM) (Pind et al, 2019), pseudospectral timedomain (PSTD) method (Hornikx et al, 2015;Hornikx et al, 2016), and adaptive rectangular decomposition (ARD) method (Mehra et al, 2012;Morales et al, 2015;Rabisse et al, 2019). They respectively offer several benefits in terms of ease of coding and applicability of complex geometries and so on according to fundamental algorithms of numerical methods.…”
Section: Introductionmentioning
confidence: 99%
“…A wide variety of numerical methods are available for timedomain simulations: finite-difference time-domain (FDTD) (Sakamoto, 2007;Kowalczyk and van Walstijn, 2008;Sakamoto et al, 2008;Kowalczyk and van Walstijn, 2011;Hamilton and Bilbao, 2017;Toyoda and Eto, 2019;Cingolani et al, 2021;Toyoda and Sakayoshi, 2021) or finite-volume timedomain (FVTD) methods (Bilbao, 2013;Bilbao et al, 2016), time-domain BEM (TD-BEM) (Hargreaves and Cox, 2008), time-domain FEM (TD-FEM) (Okuzono et al, 2019;Yoshida et al, 2022), time-domain discontinuous Galerkin FEM (DG-FEM) (Simonaho et al, 2012;Wang et al, 2019;Wang and Hornikx, 2020;Pind et al, 2021), time-domain spectral element method (TD-SEM) (Pind et al, 2019), pseudospectral timedomain (PSTD) method (Hornikx et al, 2015;Hornikx et al, 2016), and adaptive rectangular decomposition (ARD) method (Mehra et al, 2012;Morales et al, 2015;Rabisse et al, 2019). They respectively offer several benefits in terms of ease of coding and applicability of complex geometries and so on according to fundamental algorithms of numerical methods.…”
Section: Introductionmentioning
confidence: 99%
“…For frequency-domain room acoustics simulation, FEM [6][7][8][9] and the boundary element method [10,11] are standard choices because they can model various sound absorbers more easily than time-domain methods can. In contrast, with the capability of obtaining the impulse response with a single computational run, the following time-domain room acoustic simulations have been developed: the finite-difference time-domain method [12][13][14][15][16], the time-domain FEM [3,[17][18][19], the finite-volume time-domain method [20,21], the pseudospectral time-domain method [22,23], the discontinuous Galerkin FEM [24][25][26][27], and the adaptive rectangular decomposition method [28,29]. However, acoustics simulation in a real-sized room at high frequencies must address analytical models with vast degrees of freedom (DOFs).…”
Section: Introduction 1backgroundmentioning
confidence: 99%
“…Generally, wave propagation types can be examined in different ways. These are: mechanically, acoustically and electromagnetically [1][2][3][4][5][6][7][8][9]. This work will focus on acoustic waves propagation.…”
Section: Introductionmentioning
confidence: 99%
“…In the study, he evaluated the ability of the Transmission Line Matrix method to model sound scattering by cylindrical scatterers. Rabisse [2] simulated sound propagation in a confined environment with the presence of geometrical relief on the room surfaces by combining the Adaptive Rectangular Decomposition method and the Finite-Difference Time-Domain method. Duan [3] proposed an equivalent source formulation of Closed Virtual Impedance Surface (CVIS) and calculated the radiated SPL of a spherical shell in shallow and deep sea.…”
Section: Introductionmentioning
confidence: 99%