radiography testing

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    RADIOGRAPHY

    TESTING

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    Principle of Radiography

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    Principle of Radiography

    Electromagnetic radiation of certain wavelengths

    penetrate materials and are absorbed differentially

    by different materials. The emergent radiation from the job is recorded

    normally on a film

    The film after processing is called a radiograph

    and contains the shadow image of the

    discontinuities which produce differential degree

    of darkness on the radiograph

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    ELECTROMAGNETIC SPECTRUM

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    Characteristics of X rays and Gamma

    Rays

    Capable of Penetrating most of the

    industrial materials

    Travels in straight lines

    Can affect photographic films

    Can ionize gases

    Can affect living cells

    Invisible, Odorless

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    Sources of Electromagnetic

    Radiation

    X Rays

    X ray Generator, Linear Accelerator, Betatron

    Gamma Rays

    Natural and Artificial Radioactive elements

    Natural : Radium, Polonium, Uranium, Radon

    Artificial : Iridium 192, Cobalt 60, Cesium 137

    Ytterbium 170, Thulium 169

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    X RAY

    X rays are produced when high speed

    electrons hit a material target in an

    evacuated chamber ( 10 ^ -12 to 10^ -13torr )

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    CONSTRUCTION OF

    X RAY GENERATOR

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    FOCAL SPOT

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    Parameters in X Radiography

    KVControls thickness to which can be

    radiographed

    Exposure affects the density of image in

    the radiographs

    ExposuremA * Mins

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    X RAY UNIT - CONTROLS

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    Gamma radiography

    Gamma rays are

    produced during

    radioactive decay of

    elements

    Alpha particles are

    He++

    Beta particles are (-)

    Gamma radiation is

    a electromagnetic

    radiation

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    Radioactive decay

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    RADIOACTIVE

    SOURCE CAMERA

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    GAMMA RAY

    CAMERA OPERATION

    Source in stored

    position in pig

    Source cranked partially out

    source no longer shielded

    Source in exposure

    position all the way

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    Source Pencil

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    Co 60

    Created by Neutronbombardment,

    capsuled pellet

    1.17, 1.33 MeV

    Penetration 1 - 8 steel

    Requires thick shielding Container is bulky and

    handling difficult

    Iridium 192

    Produced by neutron

    bombardment 0.31, 0.47 & 0.60 MeV

    Capsuled pellet

    Easy shielded and less

    bulky widely used

    0.253 inches thick steel

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    EXPOSURE CHART

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    Characteristics of sources

    Isotope Cobalt60 Ir 192 Cs 137c

    Half life 5.3 yrs 75 days 30 yr

    Form Co Ir CsCl

    Energy 1.33,1.17 0.45 0.66

    Practical Sources

    Ci 20 50 75Rhm 27 60 30

    Dia, app, 3 mm 3 mm 10 mm

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    Characteristics of Isotopes

    Curie is a measure of disintegration of source 1 Ci

    = 3.7 x 10 10 disintegrations per sec

    In SI System it is 1 Becquerel = 1 disintegrations /sec

    Half Life : length of time required for the activity

    to decay to one half of the original value

    Energy is expressed as KeV or MeV

    Specific Activity : Ci/ gm of isotope

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    Parameters in Gamma

    radiography Source determines the thickness limit of

    radiography

    Exposure determines the density ofradiographic image

    Exposure = Curie * min

    CurieStrength of source

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    RADIOGRAPHIC FILM

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    CHARACTERISTIC CURVE

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    FILM PROCESSING

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    ASTM Penetrameters

    Hole Type Wire Type

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    LOCATION OF PENETRAMETERS

    AWS D1.1

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    Sensitivity Level

    Equivalent

    Sensitivity %

    Quality Level T of

    Penetrameter

    Perceptible

    hole dia

    0.7 1-1T 1 1T

    1.0 1-2T 1 2T

    1.4 2-1T 2 1T

    2.0 2-2T 2 2T

    2.8 2-4T 2 4T

    4 4-2T 4 2T

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    DIN Wire Penetrameter

    DIN 1-7

    1- 3.2; 2-2.5; 3-2.0; 4-1.6;

    5-1.25; 6-1.00; 7-0.8 DIN 6-12

    6-1.00; 7-0.8; 8-0.63; 9-0.5

    10-0.4 11-0.32;120.25

    DIN 10-16

    10-0.4; 11-0.32; 12- 0.25 13-0.2

    14-0.16; 15 - 0.125 16-0.1

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    ASTM Wire Penetrameter

    SET A

    No 10.08 mm, 2-0.1,30.13 4-0.16, 5-0.2, 6-0.25

    SET BNo 6-0.25,7-0.33, 8- 0.4, 9-0.51, 10-0.64,11-0.81

    SET C

    No 11-0.81, 12-1.02, 13- 1.27, 14-1.6 15-2.03 16-2.5 SET D

    No 16-2.5 17- 3.2 18-4.06 19-5.1 20-6.4 218

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    Wire Penetrameter Sensitivity

    SENSITIVITY

    S = ( D / T ) * 100

    SSensitivity in %

    D - Dia of smallest wire seen in mm

    T

    Thickness of Job in mm

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    Effect of angle of radiation

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    RT Techniques

    Double wall Single imageSingle Wall Single Image

    Job WeldFilm Source Radiation

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    RT Techniques

    Job WeldFilm Source Radiation

    Double Wall Double Image Panoramic Exposure

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    Radiation Safety

    Radiation safety is ensured by

    Radiation Protection

    Radiation monitoring

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    Radiation Protection

    Radiation Protection is ensured by

    Undertaking RT in an enclosure

    Maintaining safe distances

    Providing local temporary enclosure around the

    source

    Retaining the source in the camera when not inuse

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    Radiation Monitoring

    Ensuring that radiation intensity

    is within limits

    Thermo Luminescent Dosage(TLD) badge is used for

    monitoring the dosage received

    by the operator

    TLD Badges are processed every

    month by BARC or its

    authorised agency

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    AWS D1.1

    RT Evaluation

    * Pl refer to codes for details

    w

    e

    ld

    s

    i

    ze

    Gap between defects

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    AWS D1.1

    RT Evaluation

    * Pl refer to codes for details

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    RADIOGRAPHIC INDICATIONS

    INTER-PASS SLAG INCLUSIONS

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    RADIOGRAPHIC INDICATIONS

    SLAG INCLUSION

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    RADIOGRAPHIC INDICATIONS

    SLAG INCLUSION

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    RADIOGRAPHIC INDICATIONS

    CLUSTER PORES

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    RADIOGRAPHIC INDICATIONS

    LACK OF PENETRATION

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    RADIOGRAPHIC INDICATIONS

    PORES

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    RADIOGRAPHIC INDICATIONS

    WORM HOLE

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    THANK YOU