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Flow Induced Oscillations of a Helmholtz Resonator. Paul E. Slaboch Advisor: Scott C. Morris. Motivation. Interior pressure oscillations are a problem for both the automotive and aerospace communities. - PowerPoint PPT Presentation
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19 October 20062006 AME Graduate Student
Conference
Flow Induced Oscillations of a Helmholtz Resonator
Paul E. Slaboch
Advisor: Scott C. Morris
20 November 20052006 AME Graduate Student
Conference
Motivation
Interior pressure oscillations are a problem for both the automotive and aerospace communities.
In automotive vehicles, the very low frequency (~14-17 Hz) high amplitude pressure oscillations can exceed 120 dB, which can be painful to both drivers and passengers.
The goal of this study is to determine the underlying flow physics of the problem and to generate design guidelines for future vehicles to minimize buffeting.
20 November 20052006 AME Graduate Student
Conference
Introduction
Helmholtz resonators occur when flow passes over an orifice, through a neck and into a volume.
The resonator can be modeled as a spring-mass system.
Uonset occurs when fn=fR
0 0
0
0
4
( 0.25 2 )
0.375 ( 1)
0.875 ( 2)
2 ( )
(when 0)2 2
n
n
n
R
R
f L cn
U U
f Ln const
U
f Ln const
U
a Sf
V l C S
a S a Sf l
VC V
20 November 20052006 AME Graduate Student
Conference
Previous Work
20 November 20052006 AME Graduate Student
Conference
Previous Work
20 November 20052006 AME Graduate Student
Conference
Experimental Setup
PIV Cameras
Cavity
Open Orifice
20 November 20052006 AME Graduate Student
Conference
Pressure Measurements
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 520
40
60
80
100
120
140
f/fHR
Cav
ity p
' (dB
)
Volume=0.1m3, Window 12.5cmx12.5cm, U=UOnset
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 220
40
60
80
100
120
140
f*L/U
Cav
ity p
' (dB
)
Volume=0.1m3, Window 12.5cmx12.5cm, U=UOnset
20 November 20052006 AME Graduate Student
Conference
Pressure Measurements
f*L/U
U/U
Ons
et
log10
(sqrt(Gpp
)/q), Volume=0.1m3, Window 12.5cmx12.5cm
0 0.5 1 1.5 20
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
-5
-4.5
-4
-3.5
-3
-2.5
-2
-1.5
-1
-0.5
0
f/fHR
U/U
Ons
et
log10
(sqrt(Gpp
)/q), Volume=0.1m3, Window 12.5cmx12.5cm
0 0.5 1 1.5 20
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
-5
-4.5
-4
-3.5
-3
-2.5
-2
-1.5
-1
-0.5
0
f*L/U
U/U
Ons
et
Cavity p' (dB), Volume=0.1m3, Window 12.5cmx12.5cm
0 0.5 1 1.5 20
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
20
40
60
80
100
120
140
f/fHR
U/U
Ons
et
Cavity p' (dB), Volume=0.1m3, Window 12.5cmx12.5cm
0 0.5 1 1.5 20
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
20
40
60
80
100
120
140
20 November 20052006 AME Graduate Student
Conference
Pressure Measurements
f*L/U
U/U
Ons
et
log10
(sqrt(Gpp
)/q), Volume=0.1m3, Window 12.5cmx12.5cm
0 0.5 1 1.5 20
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
-5
-4.5
-4
-3.5
-3
-2.5
-2
-1.5
-1
-0.5
0
20 November 20052006 AME Graduate Student
Conference
PIV Flow Visualization
20 November 20052006 AME Graduate Student
Conference
PIV Measurements
20 November 20052006 AME Graduate Student
Conference
Effect of Free Stream Velocity
20 November 20052006 AME Graduate Student
Conference
Effect of BL Thickness
20 November 20052006 AME Graduate Student
Conference
Future Work
20 November 20052006 AME Graduate Student
Conference
Future Work
20 November 20052006 AME Graduate Student
Conference
Conclusions A series of experiments has been performed to
determine the underlying flow physics of a flow induced Helmholtz resonator.
The actual mechanism of the oscillations is neither the roll up of discrete vortices nor a flag flapping shear layer instability. Rather, it appears to be a combination of the two.
The effect of free stream velocity is to spread the vorticity into a more continuous stream while the effect of the boundary layer thickness is to alter the location of the formation of a vortex.
This study, combined with future work, will provide design guidelines for automotive designers.
20 November 20052006 AME Graduate Student
Conference
Thank you for your attention.
Questions?