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Published byLeah Theobald Modified over 9 years ago
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J. Stuart Bolton Ph.D. Institute of Sound and Vibration Research, Southampton University, UK. Poroelastic materials and applied signal processing Professor of Mechanical Engineering Wave propagation and sound radiation Sound Field visualization Poroelastic materials Noise Control Americas Editor (with Patricia Davis) of the Journal of Sound and Vibration Funding from: 3M, Sony, Cummins Engines, Boeing, Raytheon Aircraft . . .
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Optimization of Acoustic Treatments
3 foams , 2 air space, 3 panel F O A M 1 2 3 AIR Panel 2 Panel 3 Panel 1 Incidence 1 Tc Transmitted Reflection Rc Area I Z=0 Z=L1 Z= L2 L3 II L4 L5 III IV V VI VII Honeycomb panel solve for Area II Area IV Panel motion Area V Area III Area VI Area VII Apply b.c.’s at each interface
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B&K Four-mic TL tube SEM – Thinsulate
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Component Noise: e.g. Tire Radiation Analysis Procedure
SPL & Sound Intensity on a hemisphere surrounding a tire [ Direct BEM ] radiation field characteristics based on Acoustic Radiation Mode (Acoustic Transfer Vector) Sound Power Radiation Efficiency Radiation Mode Contribution [ Structural Harmonic FEM ] structural wave propagation based on surface normal velocities
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Acoustical Holography for Noise Source Identification: e. g
Acoustical Holography for Noise Source Identification: e.g. rolling tire at 21 mph (128 Hz) n 3 Frequency # of nodes 164 Hz 8 (n=4) 140 Hz 6 (n=3) 115 Hz 4 (n=2) From Dispersion Curve
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