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Title: Dia 1


1
Microflown based Applications Microflown
Technologies The Netherlands www.microflown.com in
fo_at_microflown.com
2
  • Contents
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing

3
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing

4
Company Introduction
1994 Invention Microflown by Hans-Elias de Bree
at University Twente 1997 Ph.D. Hans-Elias de
Bree 1998 Founding Microflown Technologies B.V.
(de Bree, Koers) 2001 Industrializing
product 2003 Introduction broad banded sensor
element 2004 First applications scientifically
proven / first arrays sold 2005 Rapid growth in
(automotive aerospace) industry 2005 De Bree
appointed Professor Vehicle Acoustics at the
HAN University, Arnhem School of
Automotive Engineering 2008 12 FTE company 4
Ph.D. students, 1 MEURO turnover
5
Company Introduction
  • Main markets Microflown is focusing on are
    Automotive, Aerospace and Defense
  • 12 FTE Company 4 PhD students
  • lt1 million euro turnover
  • Rapidly growing company
  • Own faculty at the Han University of Automotive
    engineering in Arnhem

6
References
  • Automotive - OEM
  • Audi, BMW, DAF Paccar, Daimler, Ford,
    Freightliner, Harley Davidson, Honda, Isuzu,
    Mazda, Nissan, PSA Group ( Peugeot - Citroën ),
    Renault Samsung, Toyota, Volkswagen
  • Automotive - Others
  • AISIN, Behr Group, Eaton USA, Faurecia, Fontijne
    Grotnes, Harman Becker Automotive Systems, ISM
    Automotive, Jatco, Mirror Controls International,
    Mitsuba, Rieter Automotive, Rietschle Thomas,
    Robert Bosch, Siemens VDO, Stankiewicz
  • Aerospace
  • Aeronautical Development Establishment
    Bangalore,  Airbus France, Airbus Germany, DLR (
    German Aerospace Center ), General Electric
    Propulsion Systems, Progency Systems Corporation

7
References
  • Defense Security
  • Batelle, BBN, Dutch Ministery of Defense,
    University of the Federal Armed Forces (
    Germany), Naval Post Graduate School, Wehr
    Technische Dienst
  • Test houses
  • LMS International, Mueller-BBM, Ricardo UK,
    SPEKTRA
  • Other Industries
  • ASML, BOSE, CAE Engineering and Services, Canon,
    CNAM, EMPA, Fisher-Rosemount, INRS, INSA, KAZ,
    KNMI, Kobe Seitetsusyo, MSX International, Nippo
    Hoso Kyokai, Oticon, Pioneer, RION, Sick Maihak,
    Sony

8
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing

9
Microflown
  • Microphone measures sound pressure (result)
  • Microflown measures Particle Velocity (cause)
  • Acoustical lt-gt electrical lt-gt energy
  • Sound pressure lt-gt voltage lt-gt potential
  • Particle velocity lt-gt Amperes lt-gt kinetic

10
Microflown
PRESSURE WAVE
11
Microflown
PRESSURE WAVE ? PARTICLE VELOCITY
(Source ISVR)
12
Microflown
13
Microflown
  • Surface velocity measurement
  • No background noise problems

Figure of eight
High surface velocity and low surface pressure
Low surface velocity and high surface pressure
14
Microflown
Product range
15
Microflown
Scanning Probes
  • 1D velocity
  • For small objects
  • High temperatures

16
PU Probes
Microflown
  • Particle Velocity
  • Sound Pressure
  • 1D sound Intensity
  • Impedance
  • 1D Sound Energy

17
PU Probes Placement of p and u
Microflown
18
Microflown
Metal Mesh
  • Wind shield, DC flow till 2 m/s
  • Protection

19
USP
Microflown
  • 3D Particle Velocity
  • Sound Pressure
  • 3D sound Intensity
  • Impedance
  • 3D Sound Energy

20
Microflown
3D Sound Chip
21
Microflown
  • Calibration standing wave tube
  • Loudspeaker on one side,
  • reference pressure microphone at the other side
  • in the tube, known relation between pressure at
    the end and
  • pressure and velocity in the tube

loudspeaker
Standing wave lt-gt
Reference microphone
PU probe
22
Microflown
Calibration Piston on a sphere Known relation
between sound pressure and particle velocity in
front of the speaker. Use a reference pressure
microphone to calibrate the Microflown probe.
23
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing

24
1. Scan Listen
With the Scan Listen device p and u can be
heard directly
  • Easy finding of modes / vibration patterns
  • Easy finding of sources
  • Squeak Rattle
  • Portable
  • Simple to use

25
1. Scan Listen
26
1. Scan Listen
27
1. Scan Listen
28
1. Scan Listen
  • The setup consists of two steel plates,
  • the right one is vibrating
  • the left one is steady
  • p and u are measured at the same place on both
    plates with pu probes
  • Two measurements are done
  • without background noise
  • with background noise

Gong
pu probes
29
1. Scan Listen
Without background noise
Hard plate
Gong
30
1. Scan Listen
With background noise
Hard plate
Gong
31
Example 2 finding modeshapes
1. Scan Listen

32
Example 2 finding modeshapes
1. Scan Listen



33
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing
  • Far field Acoustic Vector Sensors

34
2. Near field acoustic camera
35
2. Near field acoustic camera
  • Features / Benefits
  • Near field method
  • Measured reliable acoustic particle velocity
    data
  • Real time visualization of all relevant acoustic
    data
  • One point methodology
  • Free configuration of measurement grid
  • Full bandwidth 20Hz-20kHz
  • Large dynamic range gt40dB
  • Low susceptibility to background noise and
    reflections
  • No need for anechoic room or in anechoic
    conditions
  • Visualization of transients
  • Non coherent noise sources
  • Multi purpose tool -gt probes can be used for
    other applications

36
2. Near field acoustic camera
Each probe measures Sound Pressure and Particle
velocity (and thus Intensity) in one
spot Velocity and Intensity are directly
determined, without complex mathematics (like
near field holography)
Microphone opening
Velocity Microflown
Mini PU probe
37
NAH Near field Acoustic Holography
2. Near field acoustic camera
  • Measure pressure and calculate the velocity
    somewhere else
  • Based on assumptions that are not met in practice
  • Very difficult method
  • - Only mid frequency
  • - Relative low dynamic range
  • Only planar or spherical sources
  • Only used as an indication
  • Results influenced by background noise or
    reflections

38
2. Near field acoustic camera
JASA paper (Jacobsen) Velocity-based
predictions were consistently found to be better
than pressure-based predictions Test setup
for ideal condition -anechoic room -semi
infinite wall -flat surface -1000
measurements Conclusion Reconstruction of
particle velocity fails
39
2. Near field acoustic camera
A simulation study radiation from a point driven
panel in a baffle
( Finn Jacobsen )
40
2. Near field acoustic camera
41
Beam forming arrays
2. Near field acoustic camera
  • Low resolution
  • Mainly suitable for high frequency
  • Relative low dynamic range
  • Results can be influenced by background noise or
    reflections
  • simple method
  • far field

42
2. Near field acoustic camera
  • SAE 2005 paper (Hald)
  • Sound intensity method has no frequency
    limitations

Beam forming
Near field holography
Intensity method
43
2. Near field acoustic camera
44
Miniature PU match Acoustic Camera
2. Near field acoustic camera
45
2. Near field acoustic camera
  • 1cm x 1cm spacing
  • Sound leak finding
  • End of line control
  • Real time movies

46
2. Near field acoustic camera
Engine run up in an engine bay (not anechoic
environment) Spacing between probes will not
result in frequency limitations. So any probe
grid configuration can be defined
PU array with flexible grid
47
2. Near field acoustic camera
Easy to deploy the measurement grid in the
software
48
2. Near field acoustic camera
49
2. Near field acoustic camera
FFT and a 3rd octave display on the left side to
show the frequency analysis of single probes in
detail
50
2. Near field acoustic camera
51
2. Near field acoustic camera
TATA Motors Noise Identification on the gear
lever panel Aim To identify the noise sources on
the Gear lever panel. The car was driven on the
test track to Identify the noise on the gear
lever panel. The measurements were done when the
vehicle was accelerated from Idle to full
throttle in 3rd gear.
52
2. Near field acoustic camera
53
(No Transcript)
54
2. Near field acoustic camera
Measuring with a portable setup inside the
Eurocopter EC 120
55
2. Near field acoustic camera
56
2. Near field acoustic camera
Case Ricardo UK
  • Replacing step scan SI sweeps for engine
    benchmarking
  • Better occupational health
  • Much faster
  • More broad banded
  • Higher spatial resolution

Ricardo UK /
57
2. Near field acoustic camera
Case Ricardo UK
FEAD Tensioner
Crank pully
Calculated Sound Power, obtained through method
utilizing the Microflown
Sound Power obtained through swept PP sound
intensity probe method
58
2. Near field acoustic camera
Case TATA Motors
TATA Motors Door Rattle Aim To locate the door
rattle noise of the left door of a Car. The
vehicle was excited on a Squeak and Rattle four
poster. The array was scanned around the door
from outside. The location of the rattle was
identified and shown.
59
2. Near field acoustic camera
Case TATA Motors
60
2. Near field acoustic camera
Case WKK
61
2. Near field acoustic camera
Case WKK
62
2. Near field acoustic camera
Case WKK
63
2. Near field acoustic camera
Case BMW
64
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing
  • Far field Acoustic Vector Sensors

65
3. Panel Noise contribution
DISPLAY
3D DIGITIZER
MEASUREMENT
66
3. Panel Noise contribution
  • Measure the contribution of each source to the
    total amount of noise at the listener position
  • Two complete separate measurements
  • Source strength measurement
  • Path measurement

67
Traditional panel noise contribution methods
3. Panel Noise contribution
  • Traditional methods
  • Two methods required for full acoustic bandwidth
  • High installation time for both methods
  • Different equipment for both methods
  • Low frequency LASER or accelerometer
  • Laser is difficult to use
  • Accelerometer massload and cable errors
  • Accelerometer high installation time,
    airborne leaks cannot be handled
  • High frequencies very much measurement points
  • High frequencies PP intensity probe
  • PP intensity probe has p/I problems
  • One need damping foam to reduce p/I problems
  • Damping foam installation is very time consuming

68
3. Panel Noise contribution
THEORY
The Kirchoff-Integral-Equation reads ...
... Since in our case no internal sources exist
...
69
3. Panel Noise contribution
THEORY
... it follows
70
3. Panel Noise contribution
THEORY
If the Greens function is now identified...
... with the reciprocally measured transfer
function P/Q ...
71
3. Panel Noise contribution
THEORY
... and the gradient ...
... with the reciprocally measured transfer
function V/Q ...
... by using
72
3. Panel Noise contribution
THEORY
... and if the pressure gradient...
... is related to the directly measured volume
velocity v...
73
3. Panel Noise contribution
THEORY
... and if ...
... is identified with the directly measured
pressure P ...
74
3. Panel Noise contribution
THEORY
... the following formula results
The right side of this formula contains only
measurable quantities (PU-sensor data).
No extra assumptions required concerning the
Greens function (like e.g. free field
condition).
75
3. Panel Noise contribution
THEORY
Approximation for hard backed wall
76
3. Panel Noise contribution
THEORY
With a discrete number of sensors
77
3. Panel Noise contribution
Transfer Functions P/Q
Microflown Sensors
78
3. Panel Noise contribution
79
3. Panel Noise contribution
Sensor mounting for PNCA measurement Decoupling
the probe from surface
80
3. Panel Noise contribution
Data hardware
81
Omnidirectional volume velocity sourcesvolume
velocity particle velocity Area
3. Panel Noise contribution
High freq. source100Hz-7kHz
Low freq. source30Hz-300Hz
82
3. Panel Noise contribution
3D DIGITIZER
83
3. Panel Noise contribution
LOADING 3D GEOMETRY MODEL
84
3. Panel Noise contribution
COMBINING MEASURED ACOUSTIC DATA ...


WITH THE 3D GEOMETRY MODEL
85
3. Panel Noise contribution
RESULTS DETAILED ANALYSIS
180 individual panel contributions
86
3. Panel Noise contribution
FREQUENCY DOMAIN
  • Frequency can be set
  • Time slot can be set
  • Display range can be set

? full flexibility
87
3. Panel Noise contribution
TIME DOMAIN
  • Frequency can be set
  • Time slot can be set
  • Display range can be set

? full flexibility
88
3. Panel Noise contribution
VALIDATION AVERAGED SPECTRA
89
3. Panel Noise contribution
Transfer Functions P/Q
Microflown Sensors
90
PNCA FEATURES
  • Unique sensor ? unique method
  • Ideal for Sound Package Optimisations or Trouble
    shooting
  • Very fast Measurement of whole vehicle
    takes max. 2 ½ days. 3D geometry
    measurement takes less than 4 hours.
  • Very flexible road measurements (wind, rain,
    gravel, etc.) are easy
  • Frequency range 100 Hz 2 kHz
  • Very high degree of detail 180 single surface
    contributions
  • Method maintains the structure and the
    absorption properties of the car. (No heavy
    spring mass system needed anymore!)

91
3. Panel Noise contribution
Helicopter interior measurements at PZL Swidnik,
Poland
92
3. Panel Noise contribution
PZL Swidnik
93
PNCA inside TGV train
3. Panel Noise contribution
94
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing

95
Traditional methods
4. In situ absorption
  • Current methods have disadvantages
  • Kundts tube
  • Sample cut-out acoustic properties are affected
  • Sound leakage due to mounting problems
  • Only under 90 degrees incidence
  • Reverberant room / alpha cabin
  • Large and expensive facilities required
  • Large samples several square meters
  • Absorption values larger than 100 is experienced
  • Microphone based free field (e.g. Tamura)
  • Large samples 10 square meter
  • Slow method 4 hour
  • Influence of background noise

96
4. In situ absorption
  • Microflown standard calibration tube can be used
    as Kundts tube
  • lower frequencies
  • can be measured
  • More accurate

97
R. Lanoye et al, a practical device to determine
the reflection coefficient of acoustic materials
in-situ based on a Microflown and microphone
sensor, ISMA, 2004.
4. In situ absorption
PU based Kundts tube method has more broadbanded
and continuous results
98
4. In situ absorption
  • Reverberant method
  • Large setup
  • Only diffuse result
  • LF problems
  • Not accurate

99
4. In situ absorption
  • Free field method Tamura
  • Free field
  • Large sample (10m2)
  • Slow method (4 hours)
  • Oblique angles possible
  • Anechoic room required

100
4. In situ absorption
  • New Microflown based method
  • In situ
  • Portable
  • Real time
  • No Kundts tube
  • Broad band 200Hz-10kHz
  • Normal and oblique angles
  • High spatial resolution
  • Flat and curved surfaces

101
4. In situ absorption
  • Impedance is the ratio of sound pressure and
    particle velocity

102
Surface impedance setup
4. In situ absorption
103
2 channel SC DAQ Surface impedance
software
4. In situ absorption
104
User-friendly software
4. In situ absorption
105
Measurementscreen
4. In situ absorption
106
Load your measurements
4. In situ absorption
107
Plot options
4. In situ absorption
108
Curve example Absorption Reflection
4. In situ absorption
109
Sample with three quarter lambda resonators
High spatial resolution
4. In situ absorption
110
4. In situ absorption
111
4. In situ absorption
112
4. In situ absorption
  • Conclusion Kundts tube
  • High flow resistivity and soft (i.e. foams)
    deviated results in the tube
  • Tubes requires uniform samples
  • Difficult materials (concrete, car parts)cannot
    be measured in a tube
  • No oblique measurements possible
  • Frequency limitation

113
25 VW GOLF test cars
4. In situ absorption
Case VW Golf carseats
114
1 reference car
4. In situ absorption
Case VW Golf carseats
115
4. In situ absorption
Reference car
25 test cars
116
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing

117
Vibration measurements
5. Non contact vibration
  • Surface velocity (vibration) measurement
  • Traditionally by laser or accelerometer
  • Also possible with microflown

118
5. Non contact vibration
  • Surface velocity (vibration) measurement
  • Laser
  • no mass load (contactless)
  • - expensive, large, not always possible (30)
  • Accelerometer
  • low cost
  • - Must be fixed to structure, cables, time
    consuming, mass load, cable induced errors

119
5. Non contact vibration
  • Surface velocity (vibration) measurement
  • Microflown
  • medium cost
  • contactless
  • all surfaces (also foam, air etc.)
  • can be done by hand (no stability problems)
  • Not affected by background noise

120
5. Non contact vibration
  • Very close to surface structural
  • velocity and acoustic particle coincide
  • Very close typical dimension of the source / 6
  • Maximum underestimation 2dB

121
5. Non contact vibration
Low frequencies
Thin steel plate

Onera (FR)
122
5. Non contact vibration
Thin steel plate

University of Twente
123
5. Non contact vibration
On foam
Rieter Automotive
124
Modes of turbo
LMS
5. Non contact vibration
High frequencies
125
  • Introduction
  • Microflowns
  • Applications
  • Scan Listen
  • Near field acoustic camera
  • Panel Noise Contribution Analysis
  • In situ absorption
  • Non contact vibration
  • End of line testing

126
6. End of line control
  • Acoustic check of products

127
6. End of line control
  • Audio example
  • background noise
  • reduction

128
6. End of line control
  • Acoustic check of products
  • Not always possible with microphone
  • Microflown no influence of background noise
  • Laser and accelerometer are difficult to use

129
Noise radiation Benefits Microflown sensor
6. End of line control
  • No influence background noise
  • Fast
  • Non contact
  • Easy to install

130
Comparison test
6. End of line control
131
6. End of line control
Comparison test Order tracking
Accelerometer
Microflown
132
Mirror Power actuatorMirror controls Int. (Eaton)
6. End of line control

133
6. End of line control
2
3
4
1
  • Not the absolute SPL but the sound quality is of
    importance
  • 6 different spectrograms with 6 different noise
    issues
  • 1) Good
  • 2) Grinding
  • 3) Waving
  • 4) Ticking
  • 5) Vibrating
  • 6) Buzzing

5
6
134
  • Are there any questions ?
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