j. stuart bolton

5
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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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 - PowerPoint PPT Presentation

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Page 1: J. Stuart Bolton

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 . . .

Page 2: J. Stuart Bolton

Optimization of Acoustic TreatmentsOptimization of Acoustic Treatments3 foams , 2 air space, 3 panel3 foams , 2 air space, 3 panel

FOAM1

FOAM2

FOAM3

AIR1

AIR2

Panel 2 Panel 3Panel 1

Incidence 1

Tc Transmitted

Reflection Rc

Area I

Z=0 Z=L1

Z=L2

Z=L3

II

Z=L4

Z=L5

III IV V VI VII

Honeycomb panel

solve for

Area I inin jP 0

Area II

Area IV

zv inzin

654321 hhhhhh CCCCCC

trtr jP 0z

v trztr

Panel motionxjk

ttxeWW ~ xjk

ppxeWW ~

654321 pppppp CCCCCC

Area V

Area III 21 11 AA

Area VI

Area VII

654321 qqqqqq CCCCCC

21 22 AA

Apply b.c.’s at each interface

Page 3: J. Stuart Bolton

SEM – ThinsulateSEM – Thinsulate

B&K Four-mic TL tubeB&K Four-mic TL tube

Page 4: J. Stuart Bolton

[ Direct BEM ]

radiation field characteristicsbased on Acoustic Radiation Mode

(Acoustic Transfer Vector)

SPL & Sound Intensity on a hemisphere surrounding a tire

Sound Power Radiation Efficiency

Radiation Mode Contribution[ Structural Harmonic FEM ]structural wave propagation

based on surface normal velocities

Component Noise: e.g. Tire Radiation Component Noise: e.g. Tire Radiation Analysis ProcedureAnalysis Procedure

Page 5: J. Stuart Bolton

Frequency # of nodes

164 Hz 8 (n=4)

140 Hz 6 (n=3)

115 Hz 4 (n=2)

n 3

From Dispersion Curve

Acoustical Holography for Noise Source Identification: Acoustical Holography for Noise Source Identification:

e.g. rolling tire at 21 mph (128 Hz)e.g. rolling tire at 21 mph (128 Hz)