10 vac statistical energy analysis -...
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![Page 1: 10 VAC Statistical Energy Analysis - vac.engr.uky.eduvac.engr.uky.edu/sites/vac/files/Webinars/10_VAC_Statistical_Energy... · David Herrin University of Kentucky An Introduction](https://reader034.vdocuments.us/reader034/viewer/2022051913/6004cc6126e12934f640fdb1/html5/thumbnails/1.jpg)
David HerrinUniversity of Kentucky
An Introduction to Statistical Energy Analysis
Vibro-Acoustics Consortium
August 17, 2020
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Vibro-Acoustics Consortium
August 17, 2020
2
• Basic Theory• Fundamentals• Measuring SEA Parameters• Examples
Overview
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Vibro-Acoustics Consortium
August 17, 2020
Room Acoustics Theory
Direct FieldReverberant Field
Direct Field Reverberant Field
𝐿 𝐿 10 logΓ
4𝜋𝑟4𝑅
𝑝 20 10 Pa𝑊 1.0 10 W
3
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Vibro-Acoustics Consortium
August 17, 2020
In the Reverberant Field
𝐿 𝐿 10 log4𝑅
𝐿 10 log𝑝𝑝
10 log𝑊𝑊 10 log
𝑅4
𝑝𝑝
Input Power
𝑊𝑊
𝑅4
𝑝𝑝
Acoustic Energy“Loss Factor”
𝑊 𝜂 𝜔𝐸
4
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Vibro-Acoustics Consortium
August 17, 2020
5
Theory Coupled Simple Oscillator
Burroughs et al., 1997
𝑀 𝑀𝐾
𝑥 𝑥
𝑅
𝐾𝐾
𝑅𝐵
Gyroscope
Power transferred from subsystem 1 to 2 (for a frequency band)
Constant which is a function of the oscillator properties
Energy in subsystems 1 and 2 (for a frequency band)
𝐹 𝑡
Assumption: Forces are assumed to be broadband and incoherent.
𝐹 𝑡𝐸 𝑀 𝑣 𝐸 𝑀 𝑣
𝑊 𝛽 𝐸 𝐸
𝑊
𝛽
𝐸 ,𝐸
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Vibro-Acoustics Consortium
August 17, 2020
6
Theory Coupled Simple Oscillator
Burroughs et al., 1997
𝑀 𝑀𝐾
𝑥 𝑥
𝑅
𝐾𝐾
𝑅𝐵
Gyroscope
• Power flow is proportional to the differences in the (modal) energies.• The constant relating the power flow to energy difference is a function of the
coupling parameters and oscillator properties.• Power flows from the oscillator with higher (modal) energy to the oscillator
with lower (modal) energy.
𝐹 𝑡 𝐹 𝑡𝐸 𝑀 𝑣 𝐸 𝑀 𝑣
𝑊 𝛽 𝐸 𝐸
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Vibro-Acoustics Consortium
August 17, 2020
7
Theory Coupled Multi-Resonant Case
Burroughs et al., 1997
𝑁 modes or oscillators 𝑁 modes or oscillators
𝐸𝐸𝑁
𝑊 𝛽 𝑁 𝑁 𝐸 𝐸
𝐸𝐸𝑁
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Vibro-Acoustics Consortium
August 17, 2020
8
Theory Coupled Multi-Resonant Case
Assumption More modes implies greater energy storage potential.
Coupling Loss Factors
Burroughs et al., 1997
𝑊 𝛽 𝑁 𝑁 𝐸 𝐸
𝑊 𝜔 𝜂 𝐸 𝜂 𝐸
𝜂𝛽 𝑁
𝜔 𝜂𝛽 𝑁
𝜔
𝜂𝑁 𝜂𝑁
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Vibro-Acoustics Consortium
August 17, 2020
9
• Basic Theory• Fundamentals• Measuring SEA Parameters• Examples
Overview
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Vibro-Acoustics Consortium
August 17, 2020
10
What is SEA?
• SEA is a lumped parameter approach for vibro-acoustic analysis that accounts for the flow of energy throughout the system based on statistical coupling of the system modes.
• Lumped parameter: each component or subsystem is a single entity having its own energy, either acoustic or vibrational.
• Energy flow: steady-state averages are determined from energy balances for each component or subsystem.
• Statistical averages: sound pressure and vibration velocity are values averaged over a band of frequencies and over space.
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Vibro-Acoustics Consortium
August 17, 2020
Frequency Averaging
0 100 200 300 400
Response
Frequency (Hz)
FE or BE
SEA
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Vibro-Acoustics Consortium
August 17, 2020
What is SEA? A Simple Example
Flexible wall, velocity 𝑣2
Cavity volume 𝑉, sound pressure 𝑝
Absorption coefficient
Physical World
Oscillating force
Sound source
SEA World
Power from force Sound Power
Power absorbedPower damped
𝐸vib 𝑚 𝑣 𝐸acoust𝑝 𝑉𝜌𝑐
Flexible Wall Acoustic Cavity
Rigid walls
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Vibro-Acoustics Consortium
August 17, 2020
Water Tank Analogy
(Usually, 𝐸 and 𝐸 are our unknowns)
𝑊 , 𝑊 ,
Known input powers
𝑁𝑁𝐸vib
𝑁𝑚 𝑣𝑁 𝐸acoust
𝑁1𝑁
𝑝 𝑉𝜌 𝑐
𝑊out,damp 𝜂𝜔 𝐸vib 𝑊out,absorb𝑆𝑐𝛼4𝑉 𝐸acoust
Wva
𝑊in,force 𝑊out,damp 𝑊va 𝑊in,sound 𝑊out,absorb 𝑊va
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Vibro-Acoustics Consortium
August 17, 2020
14
Assumptions Weak Coupling
Fahy, 1994
• Energy is uniform everywhere within a subsystem.• More energy is dissipated in a subsystem than is transmitted to other
subsystems.
Room 1 Room 2
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Vibro-Acoustics Consortium
August 17, 2020
15
YES No
Plate Beam
Assumptions Weak Coupling
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Vibro-Acoustics Consortium
August 17, 2020
Understanding Loss Factors
Fahy, 1994
Damping Loss Factor – Energy lost by structural damping and acoustic radiation damping. Coupling Loss Factor – Energy lost by transmission across a junction.
Room 1 Room 2
Energy absorbed at junction is included in the damping loss factors (not the coupling loss factor). Some damping at junctions is beneficial to SEA since it promotes weak coupling.
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Vibro-Acoustics Consortium
August 17, 2020
17
• Basic Theory• Fundamentals• Measuring SEA Parameters• Examples
Overview
![Page 18: 10 VAC Statistical Energy Analysis - vac.engr.uky.eduvac.engr.uky.edu/sites/vac/files/Webinars/10_VAC_Statistical_Energy... · David Herrin University of Kentucky An Introduction](https://reader034.vdocuments.us/reader034/viewer/2022051913/6004cc6126e12934f640fdb1/html5/thumbnails/18.jpg)
Vibro-Acoustics Consortium
August 17, 2020
18
Measuring Input Power
𝑊 Re 𝐹 𝑣∗ 𝐹 Re 𝑌
𝑌 is the mobility at the input location. Excitation Panel
AccelerometerLoad Cell Electro
Magnetic Shaker
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Vibro-Acoustics Consortium
August 17, 2020
19
Measuring Damping Loss Factors
𝜂𝛾
27.3𝑓
Accelerometer
Hammer
Decay Test
where 𝛾 is the initial slope of the transient response.
-40
-30
-20
-10
0
10
20
30
40
50
60
1.127 1.147 1.167 1.187 1.207 1.227 1.247Time (sec)
Tran
sien
t Res
pons
e (d
B)
Lyon and Dejong (1995)
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Vibro-Acoustics Consortium
August 17, 2020
Measuring Energy
20
Structural Subsystems
𝐸 𝑀 𝑉
Acoustical Subsystems𝐸
𝑉𝜌𝑐 𝑝
Electro Magnetic Shaker
Load Cell
Accelerometer
indicates spatial averaging.
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Vibro-Acoustics Consortium
August 17, 2020
Subsystem 1
Measuring Coupling Loss Factors
Subsystem 2(Heavily Damped)
𝐸 – Energy of Response Panel 𝑗 with respect to Excitation Panel 𝑖
𝑊 – Input power for subsystem 𝑖
𝜂1𝜔
𝐸𝐸
𝑊𝐸
21
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Vibro-Acoustics Consortium
August 17, 2020
Subsystem 1
Step 1 Excite Subsystem 1
Subsystem 2(Heavily Damped)
Measure accelerations (spatially average over several points) to find 𝐸 and 𝐸 .
𝜂1𝜔
𝐸𝐸
𝑊𝐸
22
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Vibro-Acoustics Consortium
August 17, 2020
Subsystem 1
Step 2 Excite Subsystem 2
Subsystem 2(Heavily Damped)
Measure 𝑊 using impedance head and 𝐸 accelerometer.
𝜂1𝜔
𝐸𝐸
𝑊𝐸
23
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Vibro-Acoustics Consortium
August 17, 2020
24
• Basic Theory• Fundamentals• Measuring SEA Parameters• Examples
Overview
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Vibro-Acoustics Consortium
August 17, 2020
7
4
1
3
2
56
5 mm Plastic
3 mm Steel
0.5 m x 0.5 m
0.7 m x 0.5 m
0.8 m x 0.1 m
0.5 m x 0.1 m
1
3
2
4
5
6
Test Article
Subsystems used for experimental SEA
25
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Vibro-Acoustics Consortium
August 17, 2020
26
VA-One Model
Measured Coupling Loss Factors
Measured Input Power
Semi Infinite Fluid
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Vibro-Acoustics Consortium
August 17, 2020
1.E-15
1.E-14
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
Ener
gy (N
-m)
Frequency (Hz)
Measurement
SimulationExcitation
Response
Single Input Flexural Energy
27
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Vibro-Acoustics Consortium
August 17, 2020
1.E-15
1.E-14
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
Ener
gy (N
-m)
Frequency (Hz)
Measurement
Simulation Excitation
Response
Single Input Flexural Energy
28
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Vibro-Acoustics Consortium
August 17, 2020
Single Input Flexural Energy
Excitation
Response
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
Ener
gy (N
-m)
Frequency (Hz)
MeasurementSimulation
29
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Vibro-Acoustics Consortium
August 17, 2020
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
1.E-06
1.E-05
Ener
gy (N
-m)
Frequency (Hz)
Measurement
Simulation
Response
Two Inputs Flexural Energy
Excitation
Excitation
30
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Vibro-Acoustics Consortium
August 17, 2020
Two Inputs Flexural Energy
1.E-13
1.E-12
1.E-11
1.E-10
1.E-09
1.E-08
1.E-07
1.E-06
1.E-05
Ener
gy (N
-m)
Frequency (Hz)
Measurement
Simulation
Response
Excitation
Excitation
31
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Vibro-Acoustics Consortium
August 17, 2020
Experiment Setup
• Electromagnetic shaker is attached on steel panel as input source• Average sound pressure level inside the acoustic cavity is measured• Radiated sound power from one side of the enclosure is measured
Electro Magnetic Shaker
62 4
3
57
Radiated Power1
Impedance Head
32
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Cavity Sound Pressure Level Comparison
30
40
50
60
70
80
Soun
d Pr
essu
re L
evel
(dB)
Frequency (Hz)
Measurement
Simulation
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Radiated Sound Power Level Comparison
0
10
20
30
40
50
60
Soun
d Po
wer
Lev
el (d
B)
Frequency (Hz)
MeasurementSimulation
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Treatment 1 Structural Damping
• Damping applied on panels 1, 2, and 6.
62 4
3
57
Radiated Power1
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0
10
20
30
40
50
60
Soun
d Po
wer
Lev
el (d
B)
Frequency (Hz)
BaselinePanel 1 Extra DampingPanel 2 Extra DampingPanel 6 Extra Damping
Treatment 1 Structural Damping
Simulation
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Vibro-Acoustics Consortium
August 17, 2020
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0
10
20
30
40
50
60
Soun
d Po
wer
Lev
el (d
B)
Frequency (Hz)
BaselinePanel 1 Extra DampingPanel 2 Extra DampingPanel 6 Extra Damping
Measurement
Treatment 1 Structural Damping
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Sound Absorbing Material
1 inchFiber
attached inside cavity
Treatment 2 Sound Absorption
Leak Path
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Disconnect SIF from cavityCavity gap is blocked by lagging material
Treatment 3 Barrier in Leak
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Effect of Acoustical Treatments
0
10
20
30
40
50
60
Soun
d Po
wer
Lev
el (d
B)
Frequency (Hz)
BaselineAbsorptive LiningBarrier Material
Simulation
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0
10
20
30
40
50
60
Soun
d Po
wer
Lev
el (d
B)
Frequency (Hz)
Baseline
Absorptive Lining
Barrier Material
Effect of Acoustical Treatments
Measurement
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Experiment Sample Boxes
19.6 x 19.6 in2
(1/16 in steel)
36 x 36 x 36 in3 wood box(1/2 inch thick)
26.4 x 19.6 x 19.6 in3 steel box
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Experiment Approach
• Upper box rests on lower box.• Source is placed in the lower box.• Average sound pressure level
(SPL) of two boxes measured.
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Experiment Approach
• Loudspeaker source placed in larger box.• Two microphones roved inside of boxes to identify spatially averaged SPL.
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Noise Reduction Comparison
0
10
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50
160 200 250 315 400 500 630 800 1000 1250 1600 2000 2500 3150 4000
Noi
se R
educ
tion
(dB)
Frequency (Hz)
Experiment
Simulation SEA
Simulation FEM
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SEA Model (No Flanking Path)
Diffuse Acoustic
Field
Simulation SEA VA One
SEA Model (With Flanking Path)
Diffuse Acoustic
Field
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Noise Reduction Comparison
0
10
20
30
40
50
160 200 250 315 400 500 630 800 1000 1250 1600 2000 2500 3150 4000
Noi
se R
educ
tion
(dB)
Frequency (Hz)
ExperimentSEA (Flanking Path Included)SEA (No Flanking Path)
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• Basic Theory• Fundamentals• Measuring SEA Parameters• Examples
Overview
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References
• C. B. Burroughs, R. W. Fischer, and F. R. Kern, “An Introduction to Statistical Energy Analysis,” J. Acoust. Soc. Amer., Vol. 101, No. 4, pp. 1779-1789 (1997).
• F. J. Fahy, “Statistical Energy Analysis: A Critical Review,” Phil. Trans. R. Soc. Lond. A, Vol. 346, pp. 431-447 (1994).
• R. H. Lyon and R. G. DeJong, Theory and Application of Statistical Energy Analysis, RH Lyon Corp. (1998).
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