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acousticemissiontesting-140603033903-phpapp01
Transcript of acousticemissiontesting-140603033903-phpapp01
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6/3/2014 1Hareesha N G, Dept of Aero Engg,DSCE
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Outline
1. Acoustic Emission phenomena.2. History of Acoustic Emission from Stone Age to these days.
3. AE instrumentation:
1. Sensors, preamplifiers, cables (types, specific applications).
2. Data Acquisition systems (analog and digital, signal digitation,filtration).
4. Principals of AE data measurement and analysis.
5. Source location. Attenuation, dispersion, diffraction and scatteringphenomena.
6. AE in metals.
7. Relationship between AE and fracture mechanics parameters and effects of
AE.8. AE applications.
9. International AE standards.
10. Conclusions.
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Definition of Acoustic Emission Phenomenon
Acoustic Emission is a phenomenon ofsound and ultrasound wave radiation inmaterials undergo deformation and
fracture processes.
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Acoustic Emission InstrumentationTypical AE apparatus consist of the following components:
Sensorsused to detect AE events. Preamplifiersamplifies initial signal.
Cablestransfer signals on distances up to 200m to AE devices. Cables aretypically of coaxial type.
Data acquisition device performs filtration, signals parameters evaluation,data analysis and charting.
SensorsMain amplifiers
with filtersMeasurement CircuitryPreamplifiers
with filtersComputer
Acquisition
softwareData
storage
Data presentation
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AE Sensors
Purpose of AE sensors is to detect stress waves motion that cause a local
dynamic material displacement and convert this displacement to anelectrical signal.
AE sensors are typically piezoelectric sensors with elements maid ofspecial ceramic elements like lead zirconate titanate (PZT). Mechanicalstrain of a piezo element generates an electric signals.
Sensors may have internally installed preamplifier (integral sensors).
Other types of sensors include capacitive transducers, laserinterferometers.
Regular piezoelectric sensor Integral piezoelectric sensorPreamplifier 60 dB
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Sensors Characteristics Typical frequency range in AE applications varies between 20 kHz and 1 MHz.
Selection of a specific sensor depends on the application and type of flaws to berevealed.
There are two qualitative type of sensor according to their frequency responds:resonant and wideband sensors.
Thickness of piezoelectric element defines the resonance frequency of sensor.
Diameter defines the area over which the sensor averages surface motion.
Another important property of AE sensors includes Curie Point, the temperatureunder which piezoelectric element loses permanently its piezoelectric properties.Curie temperature varies for different ceramics from 120 to 400C0. There areceramics with over 1200C0Curie temperature.
AE signal of lead break and corresponding Power spectrum.6/3/2014 Hareesha N G, Dept of Aero Engg,DSCE 6
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Installation of Sensors on StructureType of installation and choice of couplant material is defined by a specifics of
application. Glue (superglue type) is commonly used for piping inspections.
Magnets usually used to hold sensors on metal pressure vessels. Grease and oilthen used as a couplant.
Bands used for mechanical attachment of sensors in long term applications.
Waveguides (welded or mechanically attached) used in high temperature
applications. Rolling sensors are used for inspection rotating structures.
Special Pb blankets used to protect sensors in nuclear industry.
Sensor attachedwith magnet
Pb blanket in nuclearapplications
Waveguide Rolling sensorproduces by
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AE Data Acquisition Devices
Example of AE device parameters:
16 bit, 10 MHz A/D converter.
Maximum signal amplitude 100 dBAE.
4 High Pass filters for each channel
with a range from 10 KHz to 200 KHz(under software control).
4 Low Pass filters for each channelwith a range from 100 KHz to 2.1MHz (under software control).
32 bit Digital Signal Processor.
1 Mbyte DSP and Waveform buffer.
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Principals of AE Data Measurement and
Analysis
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Threshold and Hit Definition Time (HDT)
Hit 1
Hit 1
Hit 2
Short HDT
Long HDT
Time
Voltag
eThreshold
Long HDT
Short HDT
Threshold and HDT are parameters that used for detection AE signals in traditional AE
devices. HDT: Enables the system to determine the end of a hit, close out the
measurement
process and store the measured attributes of the signal.
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Burst and Continuous AE Signals
Burst AEis a qualitative description of the discrete signal's related to
individual emission events occurring within the material.
Continuous AEis a qualitative description of the sustained signal
produced by time-overlapping signals.
AE Testing Fundamentals, Equipment, Applications , H. Vallen
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AE Parameters
Peak amplitude - The maximum of AE signal.
dB=20log10(Vmax/1volt)-preamlifier gain
EnergyIntegral of the rectified voltage signal over the duration of the AE hit.
DurationThe time from the first threshold crossing to the end of the last thresholdcrossing.
Counts
The number of AE signal exceeds threshold. Average FrequencyDetermines the average frequency in kHz over the entire AE hit.
Rise time - The time from the first threshold crossing to the maximum amplitude.
Count rate - Number of counts per time unit.
. [ ]AE counts
A F kHzDuration
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Background NoiseBackground Noise: Signals produced by causes other than acoustic emission and are not relevant to the purpose of the test
Types of noise:
Hydraulic noiseCavitations, turbulent flows, boiling of fluids and leaks.
Mechanical noiseMovement of mechanical parts in contact with the structure e.g. fretting of pressure vessels against their
supports caused by elastic expansion under pressure.
Cyclic noiseRepetitive noise such as that from reciprocating or rotating machinery.
Electro-magnetic noise.
Control of noise sources:
Rise Time DiscriminatorThere is significant difference between rise time of mechanical noise and acoustic emission.
Frequency DiscriminatorThe frequency of mechanical noise is usually lower than an acoustic emission burst from cracks.
Floating Threshold or Smart Threshold
Varies with time as a function of noise output. Used to distinguish between thebackground noise and acoustic emission events under conditions of high, varying background noise.
Time
Amp
litude
Floatingthreshold
MasterSlave TechniqueMaster sensor are mounted near the area of interest and are surrounded by slave or guard sensors.
The guard sensors eliminate noise that are generated from outside the area of interest.
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Attenuation, Dispersion, Diffraction and
Scattering PhenomenaThe following phenomena take place as AE wave propagate along the structure:
Attenuation: The decrease in AE amplitude as a stress wave propagate along a structure dueto Energy loss mechanisms, from dispersion, diffraction or scattering.
Dispersion: A phenomenon caused by the frequency dependence of speed for waves. Sound
waves are composed of different frequencies hence the speed of the wave differs for
different frequency spectrums.
Diffraction: The spreading or bending of waves passing through an aperture or around the
edge of a barrier.
Scattering: The dispersion, deflection of waves encountering a discontinuity in the material
such as holes, sharp edges, cracks inclusions etc.
Attenuation tests have to be performed on
the actual structures during their inspection. The attenuation curves allows to estimate
amplitude or energy of a signal at the at the
given the distance from the sensor.
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Source Location
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Source Location Concepts
Time difference based on threshold crossing.
Cross-correlation time difference.
Zone location.
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Linear Location Linear location is a time difference method commonly used to locate AE source
on linear structures such as pipes. It is based on the arrival time difference
between two sensors for known velocity. Sound velocity evaluated by generating signals at know distances.
1
2
distance from first hit sensorD = distance between sensors
wave velocity
d D T V
d
V
Material Effectivevelocity in athin rod [m/s]
Shear[m/s] Longitudinal[m/s]
Brass 3480 2029 4280
Steel 347 5000 3089 5739
Aluminum 5000 3129 63196/3/2014 Hareesha N G, Dept of Aero Engg,DSCE 18
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Ch 1
Ch 2
t
Normalized cross-correlation function
t )}(max{
21 )()()(
tC
ChCh
tt
dttSStC
Cross-correlation function
Cross-correlation based Location
Cross-correlation method is typically appliedfor location of continuous AE signals.
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Acoustic Emission in Metals
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Sources of AE in Metals
Microscopic sources
includes dislocation movement, interaction, annihilation, slip formation, voids nucleation,growth and interaction and many other.
Major macroscopic sources
of AE in metals are: crack jumps, plastic deformation development, fracturing and de-bonding
of hard inclusions.
..
interaction
motion
formation
..
interaction
motion
formation
Phase
changes
Possible combinations
AE SOURCES
6.9 10236
Twining
Slip
branching
development
nucleation
branching
development
nucleation
crack
formation
fracturing
bond
connection
fracturing
crack
formation
fracturing
bond
connection
fracturing
Inclusions
interaction
growth
nucleation
interaction
growth
nucleation
Micro-crack
Voids
movement
annihilation
interaction
migration
generation
nucleation
movement
annihilation
interaction
migration
generation
nucleation
Dislocations
Recrystalli-
zation
More then 80% of energy
expended on fracture in
common industrial metals
goes to development of
plastic deformation.
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Plastic Deformation Plastic deformation development is accompanied by the motion of a large numbers of dislocations.
The process by which plastic deformation is produced by dislocation motions is called slip. Thecrystallographic plane along which the dislocation line moves is called the slip plane and thedirection of movement is called the slip direction. The combination of the two is termed the slipsystem.(1)
The motion of a single vacancy and a single dislocation emits a signal of about 0.01-0.05eV. The best sensitivity of modern AE devices equals 50-100eV.
Edge dislocation Screw dislocation Mixed dislocation
Edgedislocationmotion
1 2 3 4 5
Edge and screw are the two fundamental types of dislocation.
(1)Materials Science and Engineering an
Introduction, William D. Callister, Jr.
Physical
Process
Activation
Energy (eV)
Dislocation
glide
1.2
Formation ofdislocation
8-10
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F t th t T d t I D
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Factors that Tend to Increase or Decrease
the Amplitude of AE
Nondestructive Testing Handbook, volume 6Acoustic Emission Testing, Third Edition, ASNT.
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Relationship between AE and
Fracture Mechanics Parametersand AE Effects
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M d l f AE i M t l
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Models of AE in MetalsPlastic Deformation Model
Plastic deformation model relates AE and the stress intensity factor ( ).
AE is proportional to the size of the plastic deformation zone.
Several assumptions are made in this model: (1) The material gives the highest rate of AEwhen it is loaded to the yield strain. (2) The size and shape of the plastic zone ahead of the
crack are determined from linear elastic fracture mechanics concepts.
1K
2
11
2 or 6 (plain stress or plain strain)
y
ys
Kr
(3) Strains at the crack tip vary at where r is the radial distance from the crack tip. (4)
AE count rate
volume strained between (yield strain) and (uniform strain)
p
p y u
N V
N
V
0.5r
2 22 2 4 4
2 2 4
4
4
1 1
2 2 4 4
plate thickness
V
u y
p y u
y u y u
p
K K BV r r B B K
E E E
B
K
N K
The assumptions lead to development of the following equations for the model ( )2
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Fatigue Crack Model Several models were developed to relate AE count rate with crack
propagation rate.
2' '
2
'
'
' ' '
AE count rate due to plastic deformation
AE count rate due to fracture
(1 )(1 )
mm
p p c s m
p
c
p c
K KN C K N C
RRN
N
N N N
'
'
(Eq.1) The relation between AE count rate and stress intensity factor
(Eq.2) Paris law for crack propo
AE count rate per cycle
Stress intensity factor
, constants
m
n
dadN
N A K
N
K
A n
C K
gation in fatigue
The combined contribution of both plastic deformation andfracture mechanism is as follows for plastic yielding:
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AE Effects Kaiser effect is the absence of detectable AE at a fixed sensitivity level, until
previously applied stress levels are exceeded.
Dunegan corollary states that if AE is observed prior to a previous maximumload, some type of new damage has occurred. The dunegan corollaryis usedin proof testing of pressure vessels.
Felicity effect is the presence of AE, detectable at a fixed predeterminedsensitivity level at stress levels below those previously applied. The felicityeffect is used in the testing of fiberglass vessels and storage tanks.
stress at onset of AEfelicity ratio
previous maximum stress
Kaiser effect (BCB)
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Applications
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AE I ti f P V l
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AE Inspection of Pressure Vessels
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AE Inspection of Pressure Vessels
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AE Inspection of Pressure Vessels
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AE T ti f P V l
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AE Testing of Pressure Vessels
(1)Nondestructive Testing Handbook, volume 6Acoustic Emission Testing, Third Edition, ASNT.
Pressure Policy for a New Vessel(1)
Example of Transducers Distribution on Vessel's Surface(1) Typical Results Representation of Acoustic Emission Testing (1)
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Example of Pressure Vessel Evaluation
Historic index is a ratio of average
signal strength of the last 20% or200, whichever is less, of events toaverage signal strength of all events.
N
i
i
N
Kt
i
S
S
KNNtH
1
0
1
0
)(
10
1
010
1 i
i
iav SS
(1)Nondestructive Testing Handbook, volume 6Acoustic Emission Testing, Third Edition, ASNT.
The numbers on plot correspond tosensors numbers.(1)
Nnumber of hits, S0ithe signal strength ofthe i-th event, Jspecific number of eventsK=0.8J for JN1000 and K=N-200 for N>1000
Severity is the average of tenevents having the largestnumerical value of signalstrength.
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AE Standards
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AE S d d
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AE StandardsASNT - American Society for Nondestructive Testing
ANSI/ASNT CP-189, ASNT Standard for Qualification and Certification of Nondestructive Testing Personnel.
CARP Recommended Practice for Acoustic Emission Testing of Pressurized Highway Tankers Made ofFiberglass reinforced with Balsa Cores.
Recommended Practice No. SNT-TC-1A.
Association of American Railroads
Procedure for Acoustic Emission Evaluation of Tank Cars and IM-101 tanks, Issue 1, and Annex Z thereto, Test Methods to Meet FRA Request for Draft Sill Inspection program, docket T79.20-90 (BRW) ,Preliminary 2
Compressed Gas Association
C-1, Methods for Acoustic Emission Requalification of Seamless Steel Compressed Gas Tubes.
European Committee for Standardization
DIN EN 14584, Non-Destructive TestingAcoustic EmissionExamination of Metallic Pressure Equipmentduring Proof Testing; Planar Location of AE Sources.
EN 1330-9, Non-Destructive TestingTerminologyPart 9, Terms Used in Acoustic Emission Testing.
EN 13477-1, Non-Destructive TestingAcoustic EmissionEquipment CharacterizationPart 1,Equipment Description.
EN 13477-2, Non-Destructive TestingAcoustic EmissionEquipment CharacterizationPart 2,Verification of Operating Characteristics.
EN 13554, Non-Destructive TestingAcoustic EmissionGeneral Principles.
Institute of Electrical and Electronics Engineers
IEEE C57.127, Trial-Use guide for the Detection of Acoustic Emission from Partial Discharges in Oil-Immersed Power Transformers.
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AE St d d
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AE StandardsInternational Organization for Standardization
ISO 12713, Non-Destructive Testing - Acoustic Emission InspectionPrimary Calibration ofTransducers.
ISO 12714, Non-Destructive Testing - Acoustic Emission InspectionSecondary Calibration ofAcoustic Emission Sensors.
ISO 12716, Non-Destructive Testing - Acoustic Emission InspectionVocabulary
ISO/DIS 16148, gas CylindersRefillable Seamless Steel gas CylindersAcoustic EmissionExamination (AEE) for Periodic Inspection.
Japanese Institute for Standardization
JIS Z 2342, Methods for Acoustic Testing of Pressure Vessels during Pressure Tests andClassification of Test Results.
Japanese Society for Nondestructive Inspection
NDIS 2106-79, Evaluation of performance Characteristics of Acoustic Emission TestingEquipment.
NDIS 2109-91, Methods for Absolute calibration of Acoustic Emission Transducers byReciprocity Technique.
NDIS 2412-80, Acoustic Emission Testing of Spherical Pressure Vessels of High TensileStrength Steel and Classification of Test Results.
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More educational materials on
Acoustic Emission available atwww.muravin.com
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