• ASTM E 975 : 2013 : REDLINE

    Current The latest, up-to-date edition.

    Standard Practice for X-Ray Determination of Retained Austenite in Steel with Near Random Crystallographic Orientation (Withdrawn 2022)

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    Language(s):  English

    Published date:  07-03-2013

    Publisher:  American Society for Testing and Materials

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    CONTAINED IN VOL. 03.01, 2015 Describes the determination of retained austenite phase in steel using integrated intensities (area under peak above background) of X-ray diffraction peaks using chromium K[alpha] or molybdenum K[alpha] X-radiation.

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    1.1This practice covers the determination of retained austenite phase in steel using integrated intensities (area under peak above background) of X-ray diffraction peaks using chromium Kα or molybdenum Kα X-radiation.

    1.2The method applies to carbon and alloy steels with near random crystallographic orientations of both ferrite and austenite phases.

    1.3This practice is valid for retained austenite contents from 1 % by volume and above.

    1.4If possible, X-ray diffraction peak interference from other crystalline phases such as carbides should be eliminated from the ferrite and austenite peak intensities.

    1.5Substantial alloy contents in steel cause some change in peak intensities which have not been considered in this method. Application of this method to steels with total alloy contents exceeding 15 weight % should be done with care. If necessary, the users can calculate the theoretical correction factors to account for changes in volume of the unit cells for austenite and ferrite resulting from variations in chemical composition.

    1.6Units—The values stated in inch-pound units are to be regarded as standard. The values given in parentheses are mathematical conversions to SI units that are provided for information only and are not considered standard.

    1.7This standard does not purport to address all of the safety concerns, if any, associated with its use. It is the responsibility of the user of this standard to establish appropriate safety and health practices and determine the applicability of regulatory limitations prior to use.

    TABLE 1 Calculated Theoretical Intensities Using Chromium Kα RadiationA

    hkl

    Sinθ/λ

    θ

    f

    Δf′

    Δf"

    /F/2

    LP

    P

    TB

    N2

    R

    (α iron, body-centered cubic, unit-cell dimension ao  = 2.8664Å):

    110

    0.24669

    34.41

    18.474

    −1.6

    0.9

    1142.2

    4.290

    12

    0.9577

    0.001803B

    101.5C

    200

    0.34887

    53.06

    15.218

    −1.6

    0.9

    745.0

    2.805

    6

    0.9172

    0.001803B

    20.73C

    211

    0.42728

    78.20

    13.133

    −1.6

    0.8

    534.6

    9.388

    24

    0.8784

    0.001803B

    190.8C

    (γ iron, face-centered cubic, unit-cell dimension a o  = 3.60Å):

    111

    0.24056

    33.44

    18.687

    −1.6

    0.9

    4684.4

    4.554

    8

    0.9597

    0.0004594B

    75.24C

    200

    0.27778

    39.52

    17.422

    −1.6

    0.9

    4018.3

    3.317

    6

    0.9467

    0.0004594B

    34.78C

    220

    0.39284

    64.15

    14.004

    −1.6

    0.8

    2472.0

    3.920

    12

    0.8962

    0.0004594B

    47.88C

    A  Data from “International Tables for X-Ray Crystallography,” Physical and Chemical Tables , Vol III, Kynoch Press, Birmingham, England, 1962, pp. 60, 61, 210, 213; Weighted Kα1 and Kα2 value used (λ = 2.29092Å).
    B  Temperature factor (T = e−2M) where M = B(sin 2 θ)/λ2 and 2B = 0.71. Also N is the reciprocal of the unit-cell volume.
    C  Calculated intensity includes the variables listed that change with X-ray diffraction peak position.

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    Committee E 04
    Document Type Redline
    Publisher American Society for Testing and Materials
    Status Current

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