1994
DOI: 10.1006/jcph.1994.1122
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Radiation Boundary Condition and Anisotropy Correction for Finite Difference Solutions of the Helmholtz Equation

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Cited by 34 publications
(25 citation statements)
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“…BGT conditions are widely used [19,[33][34][35]21], and have recently been generalized to convex surfaces of arbitrary shapes [12].…”
Section: Bgt Boundary Conditionsmentioning
confidence: 99%
“…BGT conditions are widely used [19,[33][34][35]21], and have recently been generalized to convex surfaces of arbitrary shapes [12].…”
Section: Bgt Boundary Conditionsmentioning
confidence: 99%
“…Nevertheless, dispersion has been largely ignored in practical implementation of artificial boundary conditions for the Euler equations of gas dynamics [5,7,25]. While boundary conditions that account for the dispersive effects of discretization have been developed in some special cases [3,24], there is no general formulation for linear hyperbolic systems such as the linearized Euler equations.…”
Section: Introductionmentioning
confidence: 99%
“…Again the exact solution cannot be obtained; hence, we cannot make a quantitative evaluation of the results and the qualitative evaluation will demonstrate the correctitude of our results. The proposed approach is solved using the Navier-Stokes equations, where the wall boundary conditions and piston source characteristics for wall-embedded pistons, Equations (15)- (16), and the outflow boundary conditions are handled using the PML and acoustic radiation conditions of Tam and Webb [23], Equations (16) and (18). Next, we study the interference of the waves of three sources when the source is characterized by low frequency (ka = 2) and high frequency (ka = 8).…”
Section: Array Of Baffled Pistonsmentioning
confidence: 99%
“…For outflow boundary, we use PML, given by (16) that is finished with the outflow boundary condition designed by Tam and Webb [23] (Equation (18)). …”
Section: Two-dimensional Nonlinear Baffled Pistonmentioning
confidence: 99%
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