NISTIR 7847
Mechanical Properties Testing for Metal
Parts Made via Additive Manufacturing: A
Review of the State of the Art of Mechanical
Property Testing
John Slotwinski
April Cooke
Shawn Moylan
NISTIR 7847
Mechanical Properties Testing for Metal
Parts Made via Additive Manufacturing: A
Review of the State of the Art of Mechanical
Property Testing
John Slotwinski
April Cooke
Shawn Moylan
Intelligent Systems Division
Engineering Laboratory
March 2012
U.S. Department of Commerce
John E. Bryson, Secretary
National Institute of Standards and Technology
Patrick D. Gallagher, Under Secretary of Commerce for Standards and Technology and Director
Certain commercial entities, equipment, or materials may be identified in this
document in order to describe an experimental procedure or concept adequately.
Such identification is not intended to imply recommendation or endorsement by the
National Institute of Standards and Technology, nor is it intended to imply that the
entities, materials, or equipment are necessarily the best available for the purpose.
National Institute of Standards and Technology IR 7847
Natl. Inst. Stand. Technol. IR 7847, 22 Pages (March, 2012)
CODEN: NTNOEF
4
TABLE OF CONTENTS
INTRODUCTION 5
Background 5
Scope 5
DEFORMATION PROPERTIES 7
General Description 7
Properties Measured 8
Specific Tests 8
Tension Tests
Compression Tests
Bearing Tests
Modulus Tests
Hardness Tests
FAILURE PROPERTIES 11
General Description 11
Properties Measured 11
Specific Tests 11
Fatigue
Fracture toughness
Crack Growth
CONCLUSIONS AND NEXT STEPs 15
ACKNOWLEDGEMENTS 16
APPENDIX A: DEFINITIONS OF MATERIAL PROPERTY TERMS 17
REFERENCES 20
5
INTRODUCTION
Background
This National Institute of Standards and Technology Internal Report (NISTIR) is the first in a series of
planned reports from the National Institute of Standards and Technology’s (NIST) Engineering
Laboratory project titled Materials Standards for Additive Manufacturing.
1
This project provides the
measurement science for the additive manufacturing industry to measure material properties in a
standardized way. Currently there are no consensus-based standards in this area, except for those
pertaining to terminology and data file formats. This project, in conjunction with NIST’s Fundamental
Measurement Science for Additive Processes project,
2
will provide the technical foundation and
documentary standards development necessary to develop new consensus-based standards. This will be
done via ASTM-International’s (hereafter referred to as ‘ASTM’) Committee F42 on Additive
Manufacturing Technologies and the newly formed International Organization for Standardization (ISO)
TC261 committee on Additive Manufacturing.
Determining the properties of the powder used for metal-based additive manufacturing, as well as the
properties of the resulting bulk metal material, is a necessary condition for industry to be able to
confidently select powder and produce consistent parts with known and predictable properties. By
2014, the project team will develop and deliver enhanced measurement techniques that support new,
standardized methods for quantifying the material properties of both the powders used for additive
manufacturing and the resulting manufactured products.
The project’s research plan includes assessments of the current state-of-the-art testing methods for
determining properties of both bulk metal materials, which is the focus of this report, and raw metal
powder, which will be reported on in mid-2012. These methods will then be evaluated for applicability
and enhanced for use on additively manufactured parts and raw additive powder. NIST’s new Direct
Metal Laser Sintering (DMLS) machine will be used to make parts, and these new methods will be
rigorously implemented. Using these enhanced methods, the sensitivity of part material properties to
variations in initial powder properties will be determined. This is a critical step necessary for
determination of scopes of relevant material standards for additive manufacturing and for the
production of additive manufacturing parts with consistent properties.
Scope
In order to perform this state-of-the-art assessment of bulk metal material property measurements in a
rational and reasonable way, the focus was on existing consensus-based standards. Careful scoping of
existing standards was first performed to ensure that the assessment was both representative of the
1
http://www.nist.gov/el/isd/sbm/matstandaddmanu.cfm
2
http://www.nist.gov/el/isd/sbm/fundmeasursci.cfm
6
state-of-the-art, and at the same time not unwieldy. To do this, three criteria were applied to determine
which standards should be included in this assessment:
Metals Only standardized methods for measuring the mechanical properties of metal parts
were included. Mechanical property measurements for non-metals such as polymers or
ceramics were excluded.
Bulk Mechanical Properties Only standardized methods for measuring bulk properties were
included. Mechanical property measurements of extremely localized properties, such as those
obtained by micro-indentation methods, were excluded. This criterion does not preclude most
standardized hardness tests, because the results of these tests are reflective of the bulk
properties of the specimen.
Focus on International Standards This was done in order to make the assessment practical. A
cursory review of standards from the major Standards Development Organizations showed that
the ASTM-International and the International Organization for Standardization mechanical
standards are representative of all the pertinent standardized mechanical testing methods.
In addition, care was taken to ensure that both all of the mechanical testing characteristics required by
the MMPDS
3
and the characteristics typically reported by the additive manufacturing original equipment
suppliers were included in the assessment. The MMPDS includes both required tests (tensile,
compression, shear, bearing, moduli) and recommended tests (tests at elevated temperatures, fatigue,
fracture toughness, crack growth [1].) EOS a German producer of additive manufacturing machines
with a significant market presence in the U.S. reports tensile strength, yield point, hardness, and
fatigue strength for their materials [2]. The criteria above were applied to a total of 86 standards 58
ASTM and 29 ISO covering the measurement of material properties.
The following is organized into two sections: (1) deformation properties (where the tests attempt to
quantify how a material will yield or deform) and (2) failure properties (where the tests attempt to
quantify the potential for the component to rupture or fail.) Deformation property tests include
tension, compression, bearing, modulus, and hardness tests. Failure property tests include fatigue,
fracture toughness, and crack growth tests. Within each of these general test classifications the most
general test is first described, followed by modified tests that have testing features or parameters that
make them distinct from the most general test.
3
The MMPDS is the Metallic Materials Properties Database and Standardization. This database replaced MIL-
HDBK-5 and is the preeminent source for aerospace component design allowables. See http://
http://projects.battelle.org/mmpds/ for further information.
7
DEFORMATION PROPERTIES
General Description
One criterion for the selection of engineering materials for particular applications is how those materials
behave when subjected to forces, since parts made from those materials will typically be subjected to
forces while in service. This is particularly true for parts and structures used in the aerospace and
biomedical industry.
If a material is subjected to a static or very slowly changing stress and that stress is applied uniformly
over a cross section of that material, then the resulting deformation behavior can be characterized by a
simple stress-strain test. The stress can be applied in several different ways relative to the sample
including tension (stretching), compression (squeezing), shear (sliding), and torsion (twisting.) The
applied stress causes a certain amount of displacement, or strain, in the test specimen. The graphical
representation of the amount of strain (on the abscissa) resulting from the applied stress (on the
ordinate) is referred to as a stress-strain diagram.
For most metals that are stressed in tension at low levels, the stress and strain are proportional to each
other and the constant of proportionality is Young’s Modulus [3]. This type of low-level stress where this
proportionality is maintained is called elastic deformation. Under elastic deformation the material
returns to its original configuration after the stress is removed. For some materials the initial elastic
portion of the stress-strain relationship is not linear; in these cases the tangent (the slope of the stress-
strain curve at a specified value of stress) and/or secant modulus (the slope of a line drawn between the
origin and a given point on the stress-strain curve) is used.
Above a certain level of strain most metal materials no longer strain elastically, and non-recoverable
(i.e., the material does not return to its original configuration when the stress is released) plastic
deformation occurs. A subset of these exhibit yield-point phenomena, where the stress-strain curve
drops precipitously from the end-point of the elastic deformation (called the upper yield point), and
then remains nearly constant for further increasing strain (called the lower yield point) before again
gradually increasing for further increases in strain [3]. If the strain is continued to even higher levels
most materials eventually fail via rupturing.
Indentation tests, which measure the resistance of a material to plastic deformation, are also included
here. These types of measures use a specified load and loading condition to force a small indenter into
the material surface. The size of the indent is then measured, from which the material hardness can be
computed. Since different hardness tests employ different indenters with different sizes and
geometries, the resulting hardness value applies only to the particular test being used. Hence hardness
measurements are mostly relative in nature [3, 4].
8
Properties Measured
Deformation property tests, which include tension, compression, modulus, and hardness tests, provide
the measured material properties listed below. Definitions for many of these terms can be found in
Appendix A.
Stress-Strain Diagram
Torque-Twist Diagram
Yield Strength
Yield Point
Tensile Strength
Rupture Strength
Upper Yield Strength
Lower Yield Strength
Compressive Strength
Bearing Strength
Ductility
Young’s Modulus
Shear Modulus
Poisson’s Ratio
Tangent Modulus
Secant Modulus
Chord Modulus
Brinell Hardness Number
Rockwell Hardness Number
Knoop Hardness Number
Vickers Hardness Number
Scleroscope Hardness Number
Webster Hardness
Indentation Hardness
Indentation Modulus
Elasto-plastic Hardness
Specific Tests
Tension Tests
ASTM E8 [5] is the basic method for uniaxial tension testing of metals at room temperatures (10 °C 38
°C). ISO 6892-1 [6] is the equivalent ISO test and includes additional test sample geometries such as
sheet and wire. Both methods give the material’s measured yield and tensile strengths. ASTM E21 [7]
and ISO 6892-2 [8] provide methods for tension test of metals at elevated temperatures (above 38 °C.)
ISO 15579 is similar to ASTM E8 and ISO 6892-1 but provides guidance for testing at low temperatures,
between 10 °C and -196 °C [9]. Guidance for tension testing of metals at cryogenic temperatures (less
than -196 °C) is covered in ASTM E1450 [10] and ISO 19819 [11].
ASTM also has two metal material tension tests, ASTM E292 [12], and ASTM E740 [13] , that are similar
to E8, except that the samples are first prepared with a notch or surface-crack before subjecting them to
tension. ASTM E292 is explicitly performed at elevated temperatures. These tests provide the test
material’s rupture strength (E292) or metal plate yield strength (E740.)
Finally, there are two ISO standards, ISO 26203 [14] and ISO 26203 [15], that describe testing of metal
sheet material at high-strain rates (10
-2
s
-1
to 10
3
s
-1
and higher), such as the testing of sheet metal for
automotive bodies. There do not appear to be any equivalent standards in ASTM.
9
Compression Tests
ASTM E9 [16] is the basic method for uniaxial compression testing of metallic samples at room
temperatures. ASTM standard practice E209 [17] is the same test performed at elevated and uniform
temperatures, up to and beyond 538 °C. There do not appear to be equivalent test standards in ISO.
Bearing Tests
ASTM E238 appears to be the only ASTM or ISO method for pin-type bearing tests [18], which
determines the bearing yield strength and bearing strength for a rectangular metal specimen containing
a hole for a bearing pin. The load on the bearing pin is increased at a rate of 0.05 bearing-strain per
minute and a plot of the bearing pin load versus bearing deformation is made. From this data the
bearing yield strength and bearing strength are determined.
Modulus Tests
ASTM E111 is the basic method for conducting modulus tests [19]; it builds on the test methods
specified in ASTM E8 for tension and E9 for compression by providing additional guidance on the
number of required trials, specimen preparation, and test temperatures. It also defines how to
determine the Young’s, Tangent, and Chord modulus values from the tension and compression test
data. ASTM E111 includes guidance for modulus measurements at both high and low temperatures.
ASTM E143 provides the basic method for measuring the shear modulus at room temperature [20].
Both of the E143 and E111 methods involve subjecting the test specimens to macroscopic tension,
compression, or twisting.
Alternatively, dynamic methods that employ more microscopic deformations may be employed. ASTM
E1875 describes a vibrational method that induces a sonic resonance throughout the entire sample,
using a variable-frequency audio oscillator to generate a sinusoidal signal and a power-amplified
transducer to convert that signal into a mechanical driving vibration [21]. A suspension-coupling system
supports the test specimen and another transducer detects the mechanical vibration in the sample. If
both the flexural mode and torsional mechanical resonances of the specimen are measureable, and if
the geometry and mass are known, then the Young’s and Shear modulus and Poisson’s Ratio can be
determined. This method includes guidance for making measurements made at room, elevated, and
very low temperatures, across the range -195 °C to 1200 °C. ASTM E1876 is similar, and is also a micro-
scale deformation method; however this test uses a more localized elastic excitation, typically generated
by an impulse tool [22]. Both E1875 and E1876 methods give the dynamic Young’s and Shear Moduli
and Poisson’s Ratio. With careful experiments, ultrasonic nondestructive testing techniques, which are
similar conceptually to E1876, can measure the various dynamic moduli and Poisson’s Ratio of a
suitably-sized metal material with a measurement uncertainty of better than 1 % (k=2) [23].
10
Hardness Tests
Hardness tests give a general indication of the strength of a material and its resistance to deformation
[3]. Hardness is not a fundamental material property, however, due to the wide variety of indenters and
a material’s resistance to indentation being dependant on the size and geometry of the indenter and the
applied load [3, 4]. Hence it is difficult to make quantified comparisons between material tests made
with different indenters. ASTM E140 [24] does provide approximate conversions of the hardness values
measured with different types of indenters.
ASTM E10 [25] and ISO 6506-1 [26] provide guidance for hardness tests of metal samples using Brinell
indenters, which are spherical in shape, at room temperatures (10 °C to 35 °C). ASTM E18 [27] and ISO
6508 [28] provide the same for Rockwell (either tungsten carbide balls (Rockwell B) or diamond
spheroconical indenters (Rockwell C) hardness tests, also at room temperatures. Knoop and Vickers
indentation tests are covered in ASTM E384 [29] and ISO 4545-1 [30] (for Knoop) and ISO 6507-1 [31] for
Knoop and Vickers, respectively. Both Knoop and Vickers indenters are pyramidal in shape, but with
different face angles.
The above methods all involve the application of a static (or quasi-static) load. ASTM E448 [32]
describes a Scleroscope Hardness measurement, which is a dynamic measurement. For this test an
indenter is dropped from a height above the metal test sample, and the magnitude of the rebound
height is used to determine the hardness. ISO 14577-1 is also an elastic method, and measures both the
plastic and elastic deformation of the metal material during application of the indenter, in order to
compute the indentation modulus and the elasto-plastic hardness [33].
Four ASTM standards also provide guidance on three hand-held instrument methods which are useful in
production environments for quality control purposes. These include the Webster [34] and Barcol
Indentation Hardness [35] (both of which are not as sensitive to material properties as Rockwell or
Brinell), and the Rockwell B-Scale Hardness, which is measured using a Newage Instrument [36]. All
three of these portable methods are only standardized in ASTM for use on aluminum materials. ASTM
E110 also includes portable hardness testers [37].
Finally, ISO Technical Report 29381 [38] summarizes the state of the art in deriving bulk material tensile
properties from the indentation response of the material. It describes three techniques: representative
stress-strain, inverse finite element analysis methods, and the use of neural networks. However, all of
these techniques assume a test piece that is free of residual stresses.
11
FAILURE PROPERTIES
General Description
Part failure is an undesirable aspect of in-service parts that is difficult to predict. A number of mostly
qualitative tests have been devised to determine a part’s or materials resistance to failure under cyclical
stress or impacts. These include impact tests and cyclical stress tests, which are often made on
specimens that include pre-made cracks. These types of tests are also useful for materials that don’t
strain well and rupture quickly under applied stress, thus making them problematic for deformation
testing.
Properties Measured
Failure property tests, which include fatigue, fracture toughness, and crack growth tests, provide the
measured material properties listed below. Definitions for many of these terms can be found in
Appendix A.
Number of Cycles to Failure
Stress/Strain Ranges
Strain Ratio
Fatigue Crack Growth Rates as a Function of Stress-Intensity Factor Range (K)
Fatigue Life
Tensile and Compressive Stresses as a Function of Number of Fatigue Cycles
Representative Cycles of Mechanical Strain Versus Stress/Temperature
Plane-Strain Fracture Toughness
Fracture Toughness
Plain-Strain Crack-Arrest Fracture Toughness
Crack-Tip Opening displacement
Absorbed Impact Energy
Specimen Residual Strength
Creep Crack Growth Rate
Threshold Stress Intensity Factor
Crack Resistance Curve
Specific Tests
Fatigue
In basic fatigue tests a test specimen is subjected to cyclical stresses (e.g., tension and compression)
until the specimen fails. ASTM E466 is the basic ASTM method for room-temperature fatigue testing of
12
metals [39] and ISO 1099 is the equivalent ISO standard test method [40], although 1099 includes
guidance on performing the tests at higher temperatures. ISO 1099 provides a quantitative measure of
the fatigue life, while E466 just determines whether a part will fail for a given set of material and testing
conditions, such as material composition, geometry, and surface condition. The basic test subjects
either un-notched or pre-notched specimens to a constant amplitude periodic axial force. ASTM E606
[41] is similar to E466, but is strain-controlled instead of force-controlled fatigue, and provides guidance
on determining the fatigue life, similar to ISO 1099. In addition, E606 determines the cyclic stresses and
strains at any time during the tests.
ASTM E647 is a fatigue test that measures the rate of crack growth in a specimen [42] and determines
the rate as a function of the stress-intensity factor range (K). The method uses cyclic loading of
notched specimens that have been pre-cracked. The crack size is measured as a function of the number
of fatigue cycles, and the crack growth rates are expressed in terms of K, which is calculated from
linear stress analysis. ISO 12108 is the equivalent ISO test [43].
ASTM E2368 is a practice for strain-controlled thermomechanical fatigue testing, which occurs when a
uniform temperature and strain field over the specimen are simultaneously varied and independently
controlled [44]. ISO 12111 is the equivalent ISO test method [45]. ASTM E2714 is the ASTM test
method for creep-fatigue testing [46]. This test determines deformation and crack formation or crack
nucleation as a result of constant-amplitude strain-controlled tests or constant-amplitude force-
controlled tests (see ASTM E606, ASTM 466, ISO 12106, and ISO 1099.) These tests are typically done at
elevated temperatures and involve sequential or simultaneous application of the loading conditions
necessary to generate cyclical deformation or damage enhanced by creep deformation or damage. The
distinction between E2714 and E466 is that E2714 involves much longer hold times. ISO 12111 is the
equivalent ISO test method for strain-controlled thermomechanical fatigue testing [45].
ASTM E2760 is the ASTM test method for creep-fatigue crack growth testing [47]. E2760 covers fatigue
cycling with long loading/unloading rates and/or hold times. This causes creep deformation in the pre-
cracked crack tip and the creep deformation is then responsible for enhanced crack growth during each
loading cycle.
ASTM E2789 is the ASTM guide for fretting fatigue testing [48]. E466 is still the basic method, but E2789
provides guidance for fatigue testing of small amplitude oscillatory tangential motion between two solid
surfaces in contact. Fretting fatigue is generally characterized by a sharp decrease in fatigue life at the
same stress level of a standard specimen. This decrease is due to the shortened time required to form a
crack and the acceleration of the crack growth under the coupling of the fretting and bulk cyclical
stresses and strains.
ISO 1143 measures the fatigue life of rotating bar bending fatigue testing [49]. This method uses metal
samples with a circular cross-section, which are rotated and subjected to a bending moment. ISO 1352
is similar to ISO 1143 but is for torque-controlled fatigue testing [50]. ISO 12106 covers fatigue testing
of metal samples where the axial-strain is controlled [51]. This is similar to ISO 1099 but is a low-cycle
13
fatigue test that is performed until specimen failure. The standard has guidance on performing the test
at both low and high temperatures.
Fracture toughness
The basic fracture toughness test subjects a pre-cracked specimen to strain, in an attempt to initiate
crack growth and fracture the material. The ability of a material to resist this fracture is a measure of its
fracture toughness. ASTM E399 [52] and E1820 [53] are the basic ASTM test methods for determining
the linear-elastic plain-strain fracture toughness of metals. The E399 test is performed on metals under
linear-elastic, plane-strain conditions using fatigue pre-cracked specimens that are subjected to a slowly
increasing crack-displacement force. ISO 12737 [54] is the equivalent ISO test method of E399. In
ASTM E1820 a precracked fatigue test specimen is loaded to induce either stable or unstable crack
extensions. ISO 12135 [55] is the ISO equivalent of E1820, and ISO 22889 is similar, but provides
guidance for specimens that are very small, and hence have size sensitivities [56]. ASTM B646 [57] is the
standard practice for fracture toughness of aluminum alloys, and provides information supplementary
to E399 on specimen size, analysis, and interpretation of results, especially for parts of varying thickness,
when aluminum alloys are tested. ASTM B645 [58] is supplementary to both E399 and B646, and is the
basic test method for plane-strain fracture toughness measurements of aluminum specimens. ASTM
B909 [59] provides additional guidance for fracture toughness tests of aluminum where complete stress
relief of the aluminum samples is not possible and ASTM E1304 covers plane-strain fracture toughness
of metal materials that have a Chevron-shaped-notch [60].
ASTM E23 contains the standard methods for absorbed impact energy measurements of notched metal
bars using both Charpy and Izod test methods [61]. These two methods have differences in the shape of
the notches, the bar holding mechanisms, the impact locations, and the sample dimensions. ASTM E23
has detailed information about testing at different temperatures. ISO 148-1 is the equivalent ISO
Charpy test [62] and in addition provides guidance on performing the test at elevated or decreased
temperatures using liquid or gaseous mediums. ISO 14556 is similar to 148-1 but is for steel materials
[63].
ASTM E1221 is the ASTM test method for determining the plane-strain crack-arrest fracture toughness
of ferritic steels [64]. There does not appear to be an equivalent ISO test. ASTM E1290 [65] is the ASTM
test method for crack-tip opening displacement (CTOD) fracture toughness measurements. This test
determines the critical CTOD values, which are used to measured cleavage crack initiation toughness for
materials that exhibit a change from ductile to brittle behavior with decreasing temperatures. Finally,
ISO 27306 is a standard method of constraint loss correction of CTOD fracture toughness for fracture
assessment of steel components [66]. Specifically, this method converts fracture toughness from
laboratory specimens to the equivalent value for structural components. There does not appear to be
an equivalent ASTM standard.
14
Crack Growth
In basic crack growth testing a pre-cracked specimen is subjected to stress, and the rate of growth of the
crack(s) is measured. ASTM has four standards that cover crack growth testing. ASTM E740 [13] is the
practice for fracture testing with surface-crack tension specimens. This practice covers the design,
preparation, and testing of surface-crack specimens, and the test is performed with a continuously
increasing force, and excludes cyclical and sustained loadings. This test determines the residual strength
of specimens with semi-elliptical or circular-segment fatigue cracks. ASTM E1457 [67] is a test method
for measurement of creep crack growth times in metal specimens. It determines the creep crack growth
in metals at elevated temperatures using pre-cracked specimens that are subjected to static or quasi-
static loading conditions. ASTM E1681 [68] is a test method for determining the threshold stress
intensity factor for environmentally-assisted cracking of metallic materials, and requires an
environmental chamber. Finally, ASTM E2472 [69] is a test method for determination of resistance to
stable crack extension under low-constraint conditions, which occurs when the crack-length-to-
thickness and uncracked-ligament-to-thickness ratios are greater than or equal to 4. This test is
performed only under a slowly increasing remote applied displacement.
15
CONCLUSIONS AND NEXT STEPS
As mentioned in the introduction, this report is the first step of a longer process to develop standards
appropriate for the testing of the mechanical properties of metal parts made via additive manufacturing.
A future report will assess the practical applicability of the existing test methods and standards
summarized in this report for use on additively-made metal parts. Nevertheless, some initial
conclusions can be made.
First, this assessment shows that a large number of international, consensus-based standards covering a
wide range of material mechanical properties already exists. This is fortunate because it means that the
baseline technical development for these standard tests has already been done. These tests include the
typical mechanical properties specified in the introduction for both the MMPDS and a typical additive
parts manufacturer. The hope is that these existing tests can be used, in either their current or slightly
modified forms, on metal additive parts.
However, given the way in which these parts are manufactured, supplementary guidance will have to
accompany these tests. This will be necessary to account, for example, for the anisotropy and potential
porosity that may be present in these parts. Users should not assume that specimens made via additive
manufacturing processes are isotropic, and the influence of anisotropy and porosity on the results
obtained with these tests will need to be determined. In addition, not all of the test specimens
described in these standards are easily built with additive manufacturing; very thin test specimens for
example will be problematic because the resulting residual stresses may warp the specimens. Finally,
there is a strong need for a careful study of the sensitivity of the material properties to both the additive
manufacturing build parameters and the properties of the initial powder.
The next step is to assess the state-of-the-art measurements for the properties of metal powders. The
properties of interest include measurements of particulate size, powder chemical composition, powder
viscosity, and powder particulate morphology. This will be reported on in mid-2012. Following that, the
suitability of these existing measurements - both mechanical properties of metal parts and properties of
metal powders - will be assessed for use in additive manufacturing.
16
ACKNOWLEDGEMENTS
The authors would like to thank William Luecke (NIST/Metallurgy Division) and David McColskey
(NIST/Materials Reliability Division) for their helpful comments, suggestions, and discussions.
17
APPENDIX A: DEFINITIONS OF MATERIAL PROPERTY TERMS
Absorbed Impact Energy In an Izod or Charpy test, the amount of energy required to fracture a
material.
Bearing StrengthThe maximum bearing stress which a material is capable of sustaining. [70]
Brinell Hardness Number Result from indentation hardness test in which a number proportional to the
quotient obtained by dividing the test force by the curved surface area of the indentation which is
assumed to be spherical and of the diameter of the ball. [70]
Chord Modulus The slope of the chord drawn between any two specified points on the stress-strain
curve. [19]
Compressive StrengthThe maximum compressive stress that a material is capable of sustaining. [70]
Crack-Tip Opening Displacement The crack displacement resulting from the total deformation (elastic
plus plastic) at variously defined locations near the original (prior to force application) crack tip. [71]
Creep Crack Growth Rate The rate of crack extension caused by creep damage and expressed in terms
of average crack extension per unit time. [71]
DuctilityThe ability of a material to deform plastically before fracturing. [70]
Elasto-plastic Hardness Hardness measured from the recorded time record of the force and
displacement data of an indentation during plastic and elastic deformation.
Fatigue Cycle One complete sequence of values of force (strain) that is repeated under constant
amplitude loading (straining). [
71]
Fatigue LifeThe number of cycles of a specified character that a given specimen sustains before failure
of a specified nature occurs. [
71]
Fracture ToughnessA generic term for measures of resistance to extension of a crack. [71]
Indentation Hardness The hardness as evaluated from measurements of area or depth of the
indentation made by pressing a specific indenter into the surface of a material under specified static
loading conditions. [
70]
18
Indentation ModulusModulus measured from the recorded time record of the force and displacement
data of an indentation during plastic and elastic deformation.
Knoop Hardness Number A number related to the applied force and to the projected area of the
permanent impression made by a rhombic-based pyramidal diamond indenter having included edge
angles of 172° 30 and 130° 0. [
70]
Lower Yield Strength The minimum stress recorded during discontinuous yielding, ignoring transient
effects. [
70]
Plane-Strain Fracture Toughness The crack-extension resistance under conditions of crack-tip plane
strain in Mode I for slow rates of loading under predominately linear-elastic conditions and negligible
plastic-zone adjustment. [
71]
Poisson’s RatioThe negative of the ratio of transverse strain to the corresponding axial strain resulting
from an axial stress below the proportional limit of the material. [
70]
Rockwell Hardness Number A number derived from the net increase in the depth of indentation as the
force on an indenter is increased from a specified preliminary test force to a specified total test force
and then returned to the preliminary test force. [
70]
Rupture Strength The stress at which rupture (a failure that is accompanied by significant plastic
deformation, often associated with creep failure) occurs. [
3]
Scleroscope Hardness NumberA number related to the height of rebound of a diamond-tipped
hammer dropped on a material being tested. [
70]
Secant Modulus On a stress-strain curve, the slope of a line between the origin and any specified
stress. [
3]
Shear Modulus (aka torsional modulus) The ratio of shear stress to corresponding shear strain below
the proportional limit. [
70]
Strain Ratio The ratio of width to thickness strain determined in the uniform elongation portion of a
tension test. [
72]
Stress-Intensity Factor The magnitude of the mathematically ideal, crack-tip stress field for a particular
mode in a homogeneous, linear-elastic body. [
71]
Stress-Intensity Factor RangeIn fatigue, the variation in the stress-intensity factor in a cycle. [71]
19
Stress-Strain Diagram (aka Stress-Strain Curve) A diagram in which corresponding values of stress and
strain are plotted against each other. Values of stress are usually plotted as ordinates and values of
strain as abscissas. [
70]
Tangent ModulusThe slope of the stress-strain curve at any specified stress or strain. [19]
Tensile Strength (aka Ultimate Tensile Strength) The maximum tensile stress which a material is
capable of sustaining. Tensile strength is calculated from the maximum force during a tension test
carried to rupture and the original cross-sectional area of the specimen. [
70]
Torque-Twist Diagram (aka Torque-Twist Curve) In shear testing, a diagram in which corresponding
values of torque and twist are plotted against each other. Values of torque are usually plotted as
ordinates and values of twist as abscissas.
Upper Yield StrengthSee Yield Point.
Vickers Hardness Number A number related to the applied force and the surface area of the
permanent impression made by a square-based pyramidal diamond indenter having included face
angles of 136°. [
70]
Webster Hardness A hardness number measured by a Webster Hardness gauge. Webster Hardness
gauges can measure a range of hardness that corresponds to 5 HRE to 110 HRE on the Rockwell
hardness scale. [
34]
Yield Point (aka Upper Yield Strength) In a uniaxial test, the first stress maximum associated with
discontinuous yielding at or near the onset of plastic deformation. [
70]
Yield Strength The engineering stress at which it is considered that plastic elongation of the material
has commenced. [
70]
Young’s Modulus The ratio of tensile or compressive stress to corresponding strain below the
proportional limit of the material. [
70]
20
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21
[33] ISO, 14577-1: Metallic materials -- Instrumented indentation test for hardness and materials
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[64] ASTM, E1221: Test Method for Determining Plane-Strain Crack-Arrest Fracture Toughness, Ia, of
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22
[65] ASTM, E1290: Test Method for Crack-Tip Opening Displacement (CTOD) Fracture Toughness
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[66] ISO, 27306: Metallic materials -- Method of constraint loss correction of CTOD fracture toughness
for fracture assessment of steel components. (2009).
[67] ASTM, E1457: Test Method for Measurement of Creep Crack Growth Times in Metals. (2007).
[68] ASTM, E1681: Test Method for Determining Threshold Stress Intensity Factor for Environment-
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[69] ASTM, E2472: Test Method for Determination of Resistance to Stable Crack Extension under Low-
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[70] ASTM, E6: Terminology Relating to Methods of Mechanical Testing. (2009).
[71] ASTM, E1823: Terminology Relating to Fatigue and Fracture Testing. (2010).
[72] online:
http://www.worthingtonsteel.com. Accessed