A New Technique to Identify Arbitrarily Shaped Noise Sources
Author(s) -
Roberto A. Tenenbaum,
Marcelo Bruno S. Magalhães
Publication year - 2006
Publication title -
shock and vibration
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.418
H-Index - 45
eISSN - 1875-9203
pISSN - 1070-9622
DOI - 10.1155/2006/231625
Subject(s) - supersonic speed , sound intensity , singular value decomposition , intensity (physics) , helmholtz free energy , acoustics , operator (biology) , discretization , helmholtz equation , wavenumber , sound pressure , physics , plane (geometry) , noise (video) , field (mathematics) , acoustic radiation , aeroacoustics , mathematical analysis , mathematics , boundary value problem , radiation , geometry , optics , computer science , mechanics , algorithm , sound (geography) , repressor , artificial intelligence , image (mathematics) , chemistry , biochemistry , quantum mechanics , transcription factor , pure mathematics , gene
Acoustic intensity is one of the available tools for evaluating sound radiation from vibrating bodies. Active intensity may, in some situations, not give a faithful insight about how much energy is in fact carried into the far field. It was then proposed a new parameter, the supersonic acoustic intensity, which takes into account only the intensity generated by components having a smaller wavenumber than the acoustic one. However, the method is only efective for simple sources, such as plane plates, cylinders and spheres. This work presents a new technique, based on the Boundary Elements Method and the Singular Value Decomposition, to compute the supersonic acoustic intensity for arbitrarily shaped sources. The technique is based in the Kirchoff-Helmholtz equation in a discretized approach, leading to a radiation operator that relates the normal velocity on the source's surface mesh with the pressure at grid points located in the field. Then, the singular value decomposition technique is set to the radiation operator and a cutoff criterion is applied to remove non propagating components. Some numerical examples are presented
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