Basic principles of ultrasonic testing презентация

Содержание

Krautkramer NDT Ultrasonic Systems Examples of oscillation ball on a spring pendulum rotating earth

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Basic Principles of
Ultrasonic Testing

Theory and Practice


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Examples of oscillation
ball on a spring
pendulum
rotating earth


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The ball starts to oscillate as soon as

it is pushed

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Movement of the ball over time


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Time
One full oscillation T

Frequency
From the duration of one

oscillation T the frequency f (number of oscillations per second) is calculated:

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180
360
90
270
Phase
Time
a
0
The actual displacement a is termed as:


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Spectrum of sound
Frequency range Hz
Description
Example
0 - 20
Infrasound
Earth quake
20

- 20.000

Audible sound

Speech, music

> 20.000

Ultrasound

Bat, Quartz crystal


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gas
liquid
solid
Atomic structures
low density
weak bonding forces
medium density
medium bonding forces
high

density
strong bonding forces
crystallographic structure

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Understanding wave propagation:





Spring = elastic bonding force
Ball =

atom

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T

distance travelled
start of oscillation


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T

Distance travelled
From this we derive:
or
Wave equation

During one oscillation

T the wave front propagates by the distance λ:

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Direction of oscillation
Direction of propagation
Longitudinal wave



Sound propagation


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Transverse wave
Direction of oscillation
Sound propagation


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Wave propagation
Longitudinal waves propagate in all kind of

materials.
Transverse waves only propagate in solid bodies.
Due to the different type of oscillation, transverse waves travel at lower speeds.
Sound velocity mainly depends on the density and E-modulus of the material.

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Reflection and Transmission
As soon as a sound wave

comes to a change in material characteristics ,e.g. the surface of a workpiece, or an internal inclusion, wave propagation will change too:

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Behaviour at an interface


Medium 1
Medium 2
Interface

Incoming wave


Transmitted wave
Reflected

wave

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Reflection + Transmission: Perspex - Steel

Incoming wave
Transmitted wave
Reflected

wave

Perspex

Steel





1,87

1,0

0,87





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Reflection + Transmission: Steel - Perspex




0,13
1,0
-0,87




Perspex
Steel
Incoming wave
Transmitted wave
Reflected

wave

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Amplitude of sound transmissions:
Strong reflection
Double transmission
No reflection
Single

transmission

Strong reflection with inverted phase
No transmission

Water - Steel

Copper - Steel

Steel - Air




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Piezoelectric Effect
Piezoelectrical
Crystal (Quartz)
Battery



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The crystal gets thicker, due to a distortion

of the crystal lattice



Piezoelectric Effect


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The effect inverses with polarity change


Piezoelectric Effect


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An alternating voltage generates crystal oscillations at the

frequency f







U(f)






Sound wave with frequency f





Piezoelectric Effect


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A short voltage pulse generates an oscillation at

the crystal‘s resonant
frequency f0

Short pulse
( < 1 µs )





















Piezoelectric Effect


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Reception of ultrasonic waves
A sound wave hitting a

piezoelectric crystal, induces crystal vibration which then causes electrical voltages at the crystal surfaces.



Electrical
energy

Piezoelectrical crystal

Ultrasonic wave





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Ultrasonic Probes


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RF signal (short)


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RF signal (medium)


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Sound field


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Ultrasonic Instrument


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Ultrasonic Instrument


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Ultrasonic Instrument


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Ultrasonic Instrument


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Block diagram: Ultrasonic Instrument


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Sound reflection at a flaw





Probe
Flaw
Sound travel path
Work

piece



s





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Plate testing


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0
2
4
6
8
10

s




s


Wall thickness measurement


Corrosion


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Through transmission testing


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Weld inspection


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Straight beam inspection techniques:


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surface = sound entry
backwall
flaw
1
2
water delay




Immersion testing


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