2010
DOI: 10.2514/1.45132
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Acoustic Scattering in the Time Domain Using an Equivalent Source Method

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Cited by 59 publications
(57 citation statements)
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“…This time-domain ESM did not receive much attention and was not been used for practical engineering problems until Lee et al [77][78][79] presented significant improvements of the method and revived it. Lee et al [77][78][79] used analytical formulations of the pressure gradient 80 for the boundary condition to derive a new formulation to include the effect of a uniform motion of the surface and equivalent sources and to consider the incident field generated by arbitrary moving sources such as rotor blades. They introduced a first-order shape function to discretize the source strength in time and used the SVD to improve the numerical instability issue.…”
Section: Equivalent Source Methodsmentioning
confidence: 99%
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“…This time-domain ESM did not receive much attention and was not been used for practical engineering problems until Lee et al [77][78][79] presented significant improvements of the method and revived it. Lee et al [77][78][79] used analytical formulations of the pressure gradient 80 for the boundary condition to derive a new formulation to include the effect of a uniform motion of the surface and equivalent sources and to consider the incident field generated by arbitrary moving sources such as rotor blades. They introduced a first-order shape function to discretize the source strength in time and used the SVD to improve the numerical instability issue.…”
Section: Equivalent Source Methodsmentioning
confidence: 99%
“…They introduced a first-order shape function to discretize the source strength in time and used the SVD to improve the numerical instability issue. 77 They also introduced a time-averaging algorithm to further remove the numerical instability. 78 In the time-domain ESM, the strength of equivalent sources is given as a function of time, q e (t).…”
Section: Equivalent Source Methodsmentioning
confidence: 99%
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“…In particular, meshfree methods are widely applied to solve acoustics problems, because field points used in this method are arbitrarily distributed and the approximation smoothness order is chosen with flexibility. The method of fundamental solutions (MFS) [6], the multiple-scale reproducing kernel particle method (RKPM) [7], the element-free Galerkin method (EFGM) [8], and meshfree methods [9][10][11][12] are used to address certain acoustic problems, mainly in the frequency domain, and other methods like the equivalent source method (ESM) [13][14][15] solve problems in the time domain. Moreover, there is also a kind of method The present paper is organized as follows: In Section 2, the CSPM formulations are provided to solve the acoustic wave equations.…”
Section: Introductionmentioning
confidence: 99%
“…The first point is that pressure gradient formulations were developed to solve acoustic scattering problems [4,5,6,7,8] that require the pressure gradient as the boundary condition in acoustic scattering problems rather than an indirect step in computing the acoustic velocity. Thus pressure gradient formulations are required in their own right.…”
mentioning
confidence: 99%