UT Day3

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    Copyright © 2004 WI Ltd

    Ultrasonic TestingUltrasonic TestingDay 3Day 3

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    The Phenomenon of Sound

    REFLECTIONREFRACTION

    DIFFRACTION

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    The Phenomenon of Sound

    REFLECTIONREFRACTION

    DIFFRACTION

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    Sound at an Interface

    • Sound will e either tran!mitted acro!!or reflected ac"

    #eflected

    Tran!mitted

    Interface

    $ow much i! reflected and

    tran!mitted depend! upon the

    relati%e acou!tic impedance ofthe 2 material!

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    Inclined incidence)not at *0o +

    Incident

    Tran!mitted

    The !ound i! refracted due to difference! in

    !ound %elocity in the 2 ,I--.#./T material!

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    #.-#&CTI/• nly occur! when1

    The incident angle is other than 0°

    Water 

    Steel

    Steel

    Steel

    Water 

    Steel

    03

    #efracted

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    #.-#&CTI/• nly occur! when1The incident angle is other than 0°

    Steel

    Steel

    Water 

    Steel

    03

    #efracted

    The Two Materials has different

    VELOCITIE

    No Refraction

    03

    03

    (3

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    Snell5! Law

    Material 1

    Material 2 

    2Materialin

    1Material

      Vel 

    inVel 

     RSine

     I Sine=

    Incident

    Refracted

    /ormal

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    Snell5! Law

    Perspex 

    Steel 

    20 

    48.3

    2Materialin

    1Material

      Vel 

    inVel 

     RSine

     I Sine=

    5960

    2730

    48.3

    20=

    Sine

    Sine

    4580.04580.0   =

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    Snell5! Law

    Perspex 

    Steel 

    15 

    34.4

    2Materialin

    1Material

      Vel 

    inVel 

     RSine

     I Sine=

    5960

    2730

    15=

    Sine

    Sine

    2730

    596015SinSinR   =

    565.0=SinR

    4.34=

     R

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    Snell5! LawC 

    Perspex 

    Steel 

    20 

    S

    48.3

    24

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    Snell5! Law

    Perspex 

    Steel 

    S

    C

    CC

    S

    When an incident eam of !ound

    approache! an interface of twodifferent material!1

    #.-#&CTI/ occur!

    There may e more than one wa%eform

    tran!mitted into the !econd material6

    e7ample1 Compre!!ion and Shear 

    When a wa%eform change!

    into another wa%eform1

    8,. C$&/9.

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    Snell5! Law

    Perspex 

    Steel 

    C

    CS

     CS

       C

     S

    If the angle of Incident i!

    increa!ed the angle ofrefraction al!o increa!e!

    :p to a point where the

    Compre!!ion Wa%e i! at

    *03 from the /ormal

    !0° Thi! happen! at the

    FIRT CRITICAL AN"LE

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    ;!t Critical &ngle

    27.4

    S

    33

    C  Compre!!ion wa%e refractedat *0 degree!

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    2nd Critical &ngle

    S (Surface Wave

    !0 

    Shear wa%e refracted at *0 degree!

    57 

    Shear wa%e ecome! a !urface wa%e

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    ;!t Critical &ngle Calculation

    Perspex 

    Steel C 

    5960

    2730

    90

    I=

    Sine

    Sine

    5960

    2730=SinI 

    458.0=SinI 

    26.27= I 

    S

    190 =Sin

    27.2 

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    2nd Critical &ngle Calculation

    Perspex 

    Steel 

    3240

    2730

    90

    I=

    Sine

    Sine

    3240

    2730=SinI 

    8425.0=SinI 

    4.57= I 

    S190 =Sin

    57.4

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    #st$

    %nd

    $

    &&°

    !0°

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    Summary

    • Standard angle proe! etween ;!t and

    2nd critical angle! )46(06>0+

    • Stated angle i! refracted angle in !teel

    • /o angle proe under 6 and more

    than ?01 to a%oid eing 2 wa%e! in the

    !ame material=

    C

    C S

    ne ,efect Two .choe!

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    Snell5! Law e7ample• Calculate the ;!t critical angle for a

    per!pe7@copper interface

    • A Comp per!pe7 1 2>0m@!ec

    • A Comp copper 1 4>00m@!ec

    5.355808.0

    4700

    2730===SinI