ut thickness
TRANSCRIPT
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WELCOME TO THE
UT THICKNESSCOURSE
24 Hour Course. Class Hours: 8:00am to 4:30pm.
Breaks: At the discretion of the instructor.
Lunch: 1 hour - 11:30 - 12:30 Restrooms:
Safety:
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COURSE OBJECTIVES
Purpose: Present the body of knowledge of
Ultrasonic Thickness Testing
Objective: Impart an understanding of the
following topics of UT Thickness Inspection Principals and Theory
Equipment and Materials
Techniques and Calibrations Inspection Variables
Procedures and Specifications
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STUDENT OBJECTIVES
Purpose: Learn the body of knowledgefor Ultrasonic Thickness Testing
Objectives: To achieve an
understanding of UT thicknessinspection and a proficiency in usingportable ultrasonic thickness gages fortaking thickness measurements.
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LETS GET ACQUAINTED.
Name: Company:
Job Title:
Background:
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CLASS FORMAT
Instructor led presentation of information
Informal open discussion
Ask pertinent questions
Be respectful of others
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PERSONNEL CERTIFICATION
SNT-TC-1A
NAS 410
CP 189 ISO 9712
ACCP
CSWIP CGSB
AWS-NDE
Employer Certification
Central Certification
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NDT PERSONNEL
QUALIFICATION AND
CERTIFICATION
Recommended Practice SNT-TC-1A:
Guidelines for NDT PQ&C to assist theemployer
Published by ASNT
Uniform procedures for the qualification andcertification
Satisfy the employer's specific requirements.
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QUALIFICATION AND
CERTIFICATION
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NDT NAMES
NDTNondestructive Testing
NDI Nondestructive Inspection
NDENondestructive Examination or
Evaluation
Common NamesZyglo test, Magnaflux
test, Sonic test, etc.
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ELEMENTS OF A
NONDESTRUCTIVE TEST
Source which provides a probing medium
Changes to the probing medium
Detect the changes
Record or indicate the changes Interpret the cause of the changes
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DEFINITIONS
Indication - Response from an NDT Test False - Caused by improper technique;
usually not repeatable Non-relevant - Condition in the part;
intentional or unintentional Relevant - Unintentional discontinuity in
the part
Discontinuity - An interruption in thephysical structure of the test piece that maybe intentional or unintentional
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DEFINITIONS
FlawAn unintentional discontinuity, an
imperfection; which may, or may not be,
rejectable
Rejectable Discontinuity - A flaw related to
a relevant indication that exceeds the
acceptance criteria; a rejectable, relevantindication.
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DEFINITIONS
Defecta discontinuity that will cause the
part not to be used for its original purpose.A condition that will render the part not
useable or that could cause part failure or
malfunction
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NDT Interpretation/Evaluation Flowchart
Indication
Accept Reject
Non-
Relevant?
Relevant
IndicationFalse?
Violate
Acceptance
Criteria?
Use?
No No
IgnoreNo No
Interfere
with
Inspection?
Yes
Re-Process
Yes Yes
Yes Interpretation
Evaluation
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MAJOR NDT METHODS
VT AE
PT NRT
MT TIR
UT AE
RT VAET Laser Methods
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ADVANTAGES OF NDT
All of these methods of NDT share somecommon advantages:
Increased product reliability
Increased product safety
Increased productivity
Increased profitability
Increased product serviceability
Minimized product liability
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ADVANTAGES OF NDT
However, they also share a common
limitation:
The NDT method applied, regardless ofthe equipment and materials used, will
only be as effective as the inspector skill
allows. It is not a panacea!
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ULTRASONIC INSPECTION
Inspection method using sound
Introduces high frequency sound
waves into test object.
Measures two quantities:
time for sound to travel.
amplitude of received signal.
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HISTORY
1880 Curie brothers discoveredpiezoelectricprinciple.
Certain crystals develop a voltage when
pressure is applied.
1881 Lippman discovered the piezoelectric
principle operates in reverse.
Piezoelectric crystals will change shape
when a voltage is applied.
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HISTORY (CONTINUED)
1929 Sokolov performed thru-transmission.
Continuous wave travels through material
under test.
Displays transmitted and received signals.
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HISTORY (CONTINUED)
1941 Floyd Firestone (US) and James
Sproule (England) developed pulse - echo
test instruments.
Echoes reflected from material boundaries
and discontinuities provide test signals.
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UT THICKNESS APPLICATIONS
Discontinuity detection.
Thickness measurements.
Corrosion/Erosion. Pipe Wall Thickness.
Vessel Wall Thickness.
Plastics
Precision Measurements
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UT - ADVANTAGES
Deep penetration into material. Portable equipment: battery powered.
Pulse echo requires one sided accessibility only.
Accurate for thickness measurement and
discontinuity location.
Permits volumetric examination.
Suitable for go/no-go testing: audible & visible
alarms.
No known hazards
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UT - LIMITATIONS
Test object must be able to conduct sound.
Fine grained, elastic material.
Liquid couplant is required.
Requires a trained operator.
Discontinuities just below surface may not be
detected.
Dead Zone
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WHAT IS SOUND
Mechanical energy
propagating through amaterial in the form
of pressure waves.
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UT instrument produces an electrical pulse
Transducer:
Converts electrical pulse to sound energy.which travels through the material
Returning echoes are converted back into
an electrical signal
UT instrument processes the returning
signals for display
GENERATION OF SOUND
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ULTRASONIC TESTING
Ultrasonic Transducer
Like a speaker when transmitting;
Like a microphone when receiving
Piezoelectric Effect:
Apply electrical energy, mechanical
energy is produced Apply mechanical energy, electrical
energy is produced
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PIEZOELECTRIC EFFECT
When exposed to an alternating current anelement expands and contracts
- + + - - +
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WAVE MOTION
The pressure in the sound waves displacethe molecules in the material.
Various wave modes can be generated.Longitudinal, Shear, and Surface
Wave modes are defined by their particle
motion relative to direction of sound wavetravel.
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VELOCITY
Measured in distance travelled per unit oftime.
Inches/second (in/sec)
Inches/microsecond (in/ sec) Kilometers/second (km/sec)
meters/second (m/sec)
centimeters/microsecond (cm/ sec)
Velocity is affected by temperature
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LONGITUDINAL WAVES
Also known as Compressional Waves
Particle Vibrations parallel to the direction
of wave propagation.
Propagation
Particle vibrations
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LONGITUDINAL WAVES
Alternating zones of compression (highpressure) and rarefaction (low pressure)
Propagation
Particle vibration
Travel in solids, liquids and gases.
Highest velocity of all wave modes.
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SHEAR WAVES
Vibrations at right angles to the direction of
propagation.
Finds flaws not parallel to the surface
Propagation
Particle vibration
Not used with thickness gages
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SURFACE WAVES
Elliptical vibrations
Special wave at the surface of the part
Finds cracks and scratchesNot used with thickness gages
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SOUND WAVE MEASURMENTS
Cycle: A complete repetition of particlemotion
Frequency: Number of cycles of vibration
per second
Wavelength: Distance the sound wave
travels during a cycle
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FREQUENCY
Frequency Ranges: Audible range: 20 to 20,000 Hz.
Ultrasound: above 20,000 Hz.
Commercial testing: 100 kHz to 25 MHz.
Frequency units:
Hertz (Hz): cycle per second.
Kilohertz (KHz): thousand cycles per second.
Megahertz (MHz): million cycles per second.
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WAVELENGTH
Distance sound travels during one cycle.Measured from one point on cycle to an
identical point on the next cycle.
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WAVELENGTH/ FREQUENCY
f
V
V = velocity
f = frequency
= wavelength
V = f
Frequency and wavelength are inversely
proportional frequency increases, wavelength decreases
frequency decreases, wavelength increases
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SOUND BEAM GEOMETRY
Near
Field
Far
Zone
Intensityvaries
Beam Diverges (Spreads)
Distance
Yo
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SOUND BEAM AREAS
Near Field:
Far Field:
Yo(Near Field Length): Distance
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THE SOUND BEAM
The length of the near field can be
calculated from the following formula:
V
fDN
4
2
V
fDN
4
2
Where:
N = Near Field Length (mm) f = Frequency (MHz)
D = Crystal Diameter (mm) V = Velocity (Km/sec)
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NEAR ZONE
The larger the diameter the longer thenear zone
The higher the frequency the longer the
near zone The lower the velocity the longer the near
zone
V
fDD
4
4Near Zone
22
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THE SOUND BEAM
Beam Divergence can be calculated from
the following formula:
fD
V.arcsin
221
Where:
= Beam Divergence Angle f = Frequency (MHz)
D = Crystal Diameter (mm) V = Velocity (Km/sec)
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BEAM SPREAD
The larger the diameter the less the beam spread
The higher the frequency the less the beam spread
The lower the velocity the less the beam spread
Df
KV
D
KSine or
2
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ATTENUATION
Material Loss Attenuation:Scattering of sound by grain structure of
the material.
Conversion of sound energy into heat
Sound amplitude lost due to:
Attenuation
Beam Spread.
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SOUND AT AN INTERFACE
At an acoustic interface sound will be reflected
and/or transmitted across the interface
Reflected
Transmitted
InterfaceInterface
Incident Wave
Interface: Boundary between two materials
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ACOUSTIC INTERFACE
Boundary between two materials withdifferent acoustic impedance values.
Reflected
Transmitted
Acoustic
Interface
The amount reflectedand transmitted
depends upon the
acoustic impedancesof the two materials.
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ACOUSTIC IMPEDANCE (Z)
Impedance: Opposition a material offers to thepropagation of sound travelling through thematerial.
The greater the ratio (mismatch) between the
two impedances of the materials,
The greater the percentage of sound reflected.
Z = V xV = Velocity = Density
C O C S
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REFLECTION PRINCIPLES
100%
2
12
12
ZZ
ZZRE
Formula for reflected energy (RE):
Z1 = impedance of the first material the sound is in
Z2 = impedance of the material the sound reaches
Note: Due to the Law of Conservation of Energy
Transmitted Energy = 100% - Reflected Energy
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TRANSDUCER DESIGNS FOR
THICKNESS GAGING
Single crystal: materials > 1/2 thick.
Dual crystal: corroded and erodedmaterials.
Delay line: thin materials with parallel
surfaces.
CONTACT TRANSDUCER
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CONTACT TRANSDUCER
DESIGN
Crystal thickness determines frequency of
vibrations.
Electrodes establish electrical contact
with the crystal.
Wear plate provides protective contact
surface. Damping controls crystal ringing;
absorbs rear sound waves.
SINGLE ELEMENT
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SINGLE ELEMENT
TRANSDUCER
ExternalHousing
ConnectorElectricalLeads
InnerSleeve
Backing
ActiveElement
WearPlateElectrodes
ElectricalNetwork
Used on thicker materials; > 1/2.
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DUAL ELEMENT TRANSDUCER
ExternalHousing
ConnectorAcoustic
BarrierTransmitting
Element
Receiver
Element
Delay
Material
AngularSoundPath
Test Sample
Thickness gaging of corroded and eroded
materials.
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DUAL CRYSTAL
Used to detect reflectors
approximately parallelto test surface.
Measure: Thickness
Corrosion
Erosion
Transmitter Receiver
Sound beam is reflected and refracted intothe receiving element
DUAL ELEMENT TRANSDUCER
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DUAL ELEMENT TRANSDUCERSound reflecting off of bottom of test piece
back into the transmitting side of thetransducer.
Material is too thin for the transducer
This is referred to as DOUBLING.
DUAL ELEMENT TRANSDUCER
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DUAL ELEMENT TRANSDUCER
Sound reflecting off of bottom of test piece
reflects beyond the receiving side of the
transducer.
Mode Conversion occurs
Shear Wave gives the
thickness readout.
1 TIMES THICKNESS
Material is too thick for the probe
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Introducessound perpendicular (normal) to the
test surface. Improves near surface resolution.
DELAY TRANSDUCER
Electrical connectors
Damping
Crystal
Plastic delay tip
Detection of discontinuities near test surface.
Thickness measurement of thin materials
ULTRASONIC INSTRUMENT
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ULTRASONIC INSTRUMENT
FUNCTIONS The instrument contains six basic sections:
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS
Connecting a probe and coupling it to thetest object completes the test system
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INSTRUMENT FUNCTIONSThe Power Supply provides voltage from the
AC or batteries to drive the other instrumentcircuits
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS
The clock initiates the chain of events that
results in one complete cycle of an
ultrasonic test
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS
The clock emits s trigger signals, repeated at
the pulse repetition frequency (PRF)
Depending on instrument, the PRF may be:
Set by the operator
self-adjusting/ or both
The proper PRF depends on the part
thickness
When PRF is too fast, wraparound(display
of echoes from previous test cycles) occurs
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INSTRUMENT FUNCTIONS
The clock triggers the Timebase and Pulserat regular, evenly spaced intervals
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS
The timebase initiates time/distance displayon the instruments horizontal scale
used for distance readout
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS The pulser sends initial pulse to transducer,
causing sound to enter the test object initial pulse goes through the
Receiver/Amplifier to the display
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INSTRUMENT FUNCTIONS
The Initial Pulse is a fast rising, high voltage
pulse that activates the transducer
Duration of transducer ringing determinesthe length of the dead zone
Dead zone is the depth range in the test
material where relevant indications arehidden inside the Initial Pulses indication
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INSTRUMENT FUNCTIONS
Sound travels through the test object as
time elapses along the display
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INSTRUMENT FUNCTIONS
Sound reflects from material boundariesand discontinuities
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS Transducer echo voltage is processed by the
receiver and displayed
Echo height is determined by reflected sound
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INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS
Time base Controls
Velocity Control
adjusts the amount of time displayed
along the horizontal scale to
correspond with sound travel time
through material of a particular
velocity
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS
Pulser Controls
Pulser Energy Control
adjusts the size of the Initial Pulse
Damping Control adjusts transducer performance for
resolution versus penetrating power
Note: Both Pulser Energy and Dampingaffect duration of the dead zone
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONS
Receiver processes and amplifies signals
going to the Display
Processing is provided by detector and
filter sub-circuits
Detector sub-circuit can provide choice of
various types of signal passing through the
receiverRF or Selected video mode
INSTRUMENT FUNCTIONS
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INSTRUMENT FUNCTIONSComparison of RF and all Video modes
Negative half is often used to present a more
narrow echo (better resolution) for thickness
testing
COUPLANTS
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COUPLANTS
Liquid (usually) used to exclude air fromthe path of the sound beam.
Considerations
Wetting Ability Viscosity
Reactivity
Ease of removal
Expense
TYPICAL COUPLANTS
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TYPICAL COUPLANTS
Water Oil
Cellulose and water mixture
Grease/Petroleum Jelly
Commercially preparedHigh temperature couplants
THICKNESS INSPECTION
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THICKNESS INSPECTION
Thickness inspection incorporates:
Pulse Echo Technique
Resonance Method
Measurements are made of:
Thickness of new parts Erosion / Corrosion
C SS CO S A O S
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THICKNESS CONSIDERATIONS
Calibration procedure should be followed
Couplant should be thin as possible
Part surfaces should be smooth
Part surfaces should be parallel
Gage gives reading of first large echo
Need to verify actual reflector at times A-Scan Gages provide this verification
THICKNESS CONSIDERATIONS
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THICKNESS CONSIDERATIONS
Use two point calibration when possible
Calibration block
Known, documented NIST thickness
Same material as part being inspected
Similar temperature to the part
High temperature increases part thickness Insure new reading for each location
SOUND TRAVEL GEOMETRY
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SOUND TRAVEL GEOMETRY
Digital Thickness gages measure distances to
reflectors which are parallel to the partssurface
Straight beam transducer
Dual Element transducer
Delay Transducer
BASIC TEST TECHNIQUE
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BASIC TEST TECHNIQUE
PULSE-ECHO
Test object information provided by
reflected sound energy
Individual echo signal for each reflector
perpendicular to beam axis
BASIC TEST TECHNIQUE
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BASIC TEST TECHNIQUE
PULSE-ECHO
Displayed Information: echoes reflected
from acoustic interfaces
BASIC TEST TECHNIQUE
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BASIC TEST TECHNIQUE
RESONANCE
Resonance tests are used for thickness
measurements
Continuous wave of variable frequency
Resonance occurs when material
thickness equals 1/2 of wavelength
Has been replaced by pulse-echo method Still used in aerospace for thickness
readings and bond-testing
BASIC TEST TECHNIQUE
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S C S C N QU
RESONANCE
Displayed Information is derived from
fundamental and harmonic frequencies
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DATA PRESENTATION
Display hardware
Electro-luminescent displays
Liquid crystal displays
Paper chart recorders
Digital readouts
Computer screens
DATA PRESENTATION
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DATA PRESENTATION
A-scan
horizontal scale:
displays time to
indicate distance
vertical scale:
displays
transducer output
voltage to indicate
echo amplitude
DATA PRESENTATION
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DATA PRESENTATION
Digital Readouts
B-scan
Side view of test object:
profile of interfaces
reflecting sound beam
Immersion Testing Digital Thickness Gages
Computer Applications
TIME/DISTANCE
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RELATIONSHIP
Velocity is different in different materials
Accurate calibration is crucial
Gage converts travel time to thickness
Thickness = (Velocity) (Time)2
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THICKNESS GAGING
Uses High Frequency Sound Waves
Typically 5.0 MHz thru 20.0 MHz
Longitudinal Sound Energy
Thickness Measurement From One Side
Nondestructive
PRECISION THICKNESS
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PRECISION THICKNESS
GAGING Single Element Transducers
Highly Damped, Delay Transducers
Provides High Degree Of Accuracy
New Materials for Quality Control
Metals, Plastics, Glass and Composites
CORROSION THICKNESS
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CORROSION THICKNESS
GAGING Uses Dual Element Transducers
Erosion/Corrosion
Typically on Metal
Irregular/Pitted Reflecting Surface
DUAL ELEMENT
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TRANSDUCER ON CORRODED
MATERIAL
Roof angle focuses sound at the base of
pits.
TX RX
SINGLE ELEMENT
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SINGLE ELEMENT
TRANSDUCER ON
CORRODED MATERIAL
Much of the sound is scattered away from
the transducer.
DUAL ECHO AMPLITUDES
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DUAL ECHO AMPLITUDES
First Echo is not
always the Largest
Due to: Roof Angle
Thickness
Material Velocity Delay Material
TX RX
First
Backwall
Echo
Second
Backwall
Echo
1 st Echo
2 nd Echo
DUAL ELEMENT
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DUAL ELEMENT
ADVANTAGES
Roof Angle narrows the beam for pits
High Temp. capabilities ( 1,000 F)
Separate Elements
Use Higher Initial System Gain
Better near surface Resolution
Stable Readings on Rough Entry Surfaces
CHOOSING TRANSDUCERS
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CHOOSING TRANSDUCERS
Material Carbon steel
Cast material
Aluminum
Thickness Range
Min and Max thickness
Geometry
Min Diameter
Convex/Concave Surface
Surface Condition
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TRANSDUCER CRITERIA
Frequency
Higher Frequency -- Better Resolution
Higher Frequency -- Better Sensitivity
Roof Angle
Steeper Angle Will Have Shorter Focus
Delay Material for High Temperature
THICKNESS GAGING
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THICKNESS GAGING
PERFORMANCE VARIABLES Penetration: Ability to pass through a
material interface. Improves with longer wavelength.
Wavelength increased by decreasing
frequency.
THICKNESS GAGING
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THICKNESS GAGING
PERFORMANCE VARIABLES Resolution: Ability to individually display
reflectors located at slightly differentdepths along the sound beam.
Resolution increases with an increase
in bandwidth and/or frequency.
ZERO OFFSET ERROR
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ZERO OFFSET ERROR
Incorrect Zero Offsets
With Worn Transducers
On Curved Surfaces
On Rough Surfaces
ZeroBlock
Worn Probeon CurvedPipe
WornProbeon Zeroblock
RoughSurface
ZEROOFFSET
ZERO
OFFSET
ZEROOFFSET
ZEROOFFSET
Caused by Built In Test Block
AUTO PROBE RECOGNITION
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AUTO PROBE RECOGNITION
Optimizes setup and receiver gain.
Transducer V-Path correction.
Accurate measurements over largethickness ranges.
TrueThickness
Sample
AngularSound Path
TX RX
AUTO ZERO COMPENSATION
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Measures Time Through
Transducer
Tracks Transducer Wear
Compensate For Thermal
Drift At Elevated
Temperatures
RxDelay
TxDelay
Uncouple and Press Zero Key to:
ECHO-TO-ECHO
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Standard = [1 Coating]+[1 Metal] + [1 Metal] + [1 Coating]
Measurment 2
Total Thickness
Coating and Metal
Echo-to-Echo = [-1 Coating]+[1 Me tal] + [1 M etal] + [1 Coating]Measurment 2
Thickness ofMetal Only
Coating
Metal
2 METAL
2 METALCOATING
2 METAL+2CCOATING
1st ECHO 2nd ECHO 3rd ECHO
2 METALCOATING COATING
SoundEntry
AUTOMATIC ECHO-TO-ECHO
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No Gates To Set
Gage Automatically Finds The Two
Highest Back wall Signals
Marker Indicates Detected Echoes
Users Verifies Proper Detection
MANUAL ECHO-TO-ECHO
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User Selects Detection By Adjusting:
Signal Amplitude Blanking Gate
TWO POINT CALIBRATION
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Try to Calibrate On Actual Samples
Having The Same Surface Conditions
Same Geometry
Same Material
Cal Velocity
Enter Max Sample Thickness Enter Min Sample Thickness
Cal Zero
THICKNESS GAGE
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ADVANTAGES
Size and Cost Ease of Calibration and Operation
Auto Probe Recognition
V-Path Correction
Auto Zero Compensation
Greater Data Logging Capability
Thru Paint Echo-to-Echo Measurements
Better Thickness Accuracy
THICKNESS ACCURACY
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THICKNESS ACCURACY
Thickness measurement accuracy usingA-Scan gages is dependent on:
Detection
Flanking Gate DetectionPeak Gate Detection
Screen ResolutionNumber of Pixels
FLANKING GATE DETECTION
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Accuracy Affected By:
Coupling Pressure
Echo Amplitude
Leading Edge Shape
Transducer Alignment
Front Surface
Condition
Backwall SurfaceCondition
Material Properties
SIGNAL
AMPLITUDE
AT 50dB
SIGNAL
AMPLITUDE
AT -6 dB
THRESHOLD
GATE
Detection 1
Detection 2
PEAK DETECTION
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Dual Signals Have Multiple
Peaks
Peaks Change Due To:
Transducer Alignment
Surface Condition
Coupling Pressure
Backwall Surface Condition
Grain Structure
Peak Detection Is Less Sensitive
to pits
TIME TOPEAK
PEAKSIGNAL
PEAKGATE
PEAKSIGNAL
PEAKGATE
TIME TOPEAK
ALGORITHMS AND DSP
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Leading Edge of Echo is AutomaticallyDetected
Calibrated Accuracy Maintained When Gain
Is Adjusted System Runs At Lower Gain And Yields A
Cleaner Waveform
THE WAVEFORM
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ADVANTAGE
Voids, Disbonds And Flaws Can CauseInternal Reflections
Problem Solution
Disbond Detected Disbond ReflectionBlanked Out
Disbond
SURFACE NOISE
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SU C NO S
Sound energy reflects from rough surfaces
and high impedance materials.
Rough Surface Aluminum
Problem Solution 1 Solution 2
Reading SurfaceReflections
Surface NoiseBlanked Out
Reduce Gain
GRAIN REFLECTION
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Reading GrainNoise
Grain NoiseBlanked Out
Reduce Gain
Problem Solution 1 Solution 2
Large Internal ReflectionsFrom Grain Boundaries
Can Cause False Readings
FEATURES FOR
HIGH TEMP APPLICATION
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HIGH TEMP APPLICATION
Gain Adjust (Add Gain )
Fast Update Rate (20 Reading/Sec)
Freeze Waveform
Probe Zero (Correct for Thermal Drift)
Save Data
Waveform Thickness
Gain Settings
HIGH TEMPERATURE
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COUPLING TECHNIQUES Use Appropriate Couplant for Temp Range
F-2 Medium Temps Below 260oC (500o F)
E-2 High Temp For 260 - 500oC (500-1000o F)
Apply Couplant To Transducer Tip
Use Firm Coupling Pressure
Limit Contact Time To Five Seconds
Wipe Transducer And Press Zero Key To
Compensate For Transducer Drift
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DATALOGGER INPUT
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PRE-LOAD
BARCODE WAND
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Plugs Into RS-232 Port
Reads Standard 3 of 9
(39) Labels
Internal Barcode
Software Is Standard
on All 26DL PLUSS
0.267
ID:TML 1.00
THk: 0.286
BA
RCODEWAND
*
BARCODE WAND
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Scan Barcode Tags
From Drawings
Scan Barcode Tags
Located On TheEquipment
TML: 1.000.200
TML: 6.000.285
TML: 3.000.205
TML: 4.000.236
TML: 2.000.225
TML: 9.000.210
TML: 10.000.231
TML: 7.000.300
TML: 8.000.310
TML: 5.000.241
COM PANY: XYZ CORPORATIONDESCRIPTION: REBOILER #3, BLD 14 2NDATE: 9/16/96 DRAWING: # 85236
REV: C
Build Files As You Go Jump To Scanned Location In Pre-loaded
File
INTERFACE PROGRAMS
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N C OG MS
Usually free with gage purchase Bi-directional communication
Some use standard ASCII data
Store data for future on version/import into:
Other inspection programs
Word processing software
Spread sheet programs
INTERFACE PROGRAMS
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Print/Read Files and Waveforms
Edit Files
Produce Color Reports
Create/Load Different File Formats
Create Statistics Reports
INTERFACE PROGRAM
STATISTICS
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STATISTICS
Identifier Thickness
COLOR CODED FILEPRESENTATION
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PRESENTATION
Easy Conversion Of Boiler And Grid Files
Up To Seven Different Ranges And Colors
Change Display Size and File Orientation
Show Colors only
OTHER DATAMANAGEMENT PROGRAMS
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MANAGEMENT PROGRAMS
Credo Chartex Software UK
Cortran Rios Software UK
DataMate Krautkramer USA UltraPipe Krautkramer USA
EMPRV EDS (under development) USA
EPRI Check/Works EPRI USA
IDM Exxon USA Meridium (under development) USA
PIPE Sys Atomic Software UK
Name Manufacturer Country
Keyboard Lock
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Keyboard Lock
Press
36Simultaneously
Allows the operator to lock allkeys except ON/OFF and DIFF
Press again to un-lock the keyboard.
Change Hold/Blank
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Change Hold/Blank
Press and Hold
2MEAS
Then Press
Allows the operator to
switch between the displayHOLD and the displayBLANK conditions whenno measurement is beingmade (LOS).
and release both
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