An Indirect Boundary Element Method for Computing Sound Field

Article Preview

Abstract:

Computing sound field from an arbitrary radiator is of interest in acoustics, with many significant applications, one that includes the design of classical projectors and the noise prediction of underwater vehicle. To overcome the non-uniqueness of solution at eigenfrequencies in the boundary integral equation method for structural acoustic radiation, wave superposition method is introduced to study the acoustics. In this paper, the theoretical backgrounds to the direct boundary element method and the wave superposition method are presented. The wave superposition method does not solve the Kirchoff-Helmholtz integral equation directly. In the approach a lumped parameter model is estabiled from spatially averaged quantities, and the numerical method is implemented by using the acoustic field from a series of virtual sources which are collocated near the boundary surface to replace the acoustic field of the radiator. Then the sound field over the of a pulsating sphere is calculated. Finally, comparison between the analytical and numerical results is given, and the speed of solution is investigated. The results show that the agreement between the results from the above numerical methods is excellent. The wave superposition method requires fewer elements and hence is faster, which do not need as high a mesh density as traditionally associated with BEM.

You might also be interested in these eBooks

Info:

Periodical:

Advanced Materials Research (Volumes 476-478)

Pages:

1173-1177

Citation:

Online since:

February 2012

Export:

Price:

Permissions CCC:

Permissions PLS:

Сopyright:

© 2012 Trans Tech Publications Ltd. All Rights Reserved

Share:

Citation:

[1] L. Van Buren, L. D. Luker, M. D. Jevnager and A. C. Tims: J. Acoust. Soc. Am. Vol. 73 (1983), p.2200

Google Scholar

[2] N. Kamura and T. Anano: J. Soc. Nav. Archit. Jpn. Vol. 164 (1988), p.19

Google Scholar

[3] Ansys 5.7 Theory Manual ( Ansys Inc, Canonsburg 2001)

Google Scholar

[4] S. Suzuki, S. Maruyama: J. Sound Vibrat. Vol. 130 (1989), p.79

Google Scholar

[5] L. H. Chen and D. G. Schweikert: J. Acoust. Soc. Am. Vol. 35 (1963), p.1626

Google Scholar

[6] G. Chertock: J. Acoust. Soc. Am. Vol. 36 (1964), p.1305

Google Scholar

[7] L. G. Copley: J. Acoust. Soc. Am. Vol. 41 (1967), p.807

Google Scholar

[8] H. A. Schenck: J. Acoust. Soc. Am. Vol. 44 (1968), p.41

Google Scholar

[9] A. J. Burton and G. F. Miller: Proc. R. Soc. Lond. A. Vol. 323 (1971), p.201

Google Scholar

[10] G. H. Koopmann, L. Song and J. B. Fahnline: J. Acoust. Soc. Am. Vol. 86 (1989), p.2433.

Google Scholar

[11] Michel Tran Van Nhieu: J. Acoust. Soc. Am. Vol. 96 (1994), p.1070

Google Scholar

[12] T. W. Wu: Boundary Element Acoustic: Funaments and Computer Codes (WITPress, UK 2000)

Google Scholar