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Laboratory 9: Fractography
Mechanical Metallurgy Laboratory 431303 1
T. Udomphol
LLaabboorraattoorryy 99
Fractography
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Objectives
• Students are required to achieve basic fractographic observation skills. The samples
failed under tensile, torsion, impact or fatigue will be investigated using visual
inspection and equipments such as stereoscope, optical microscope and electron
microscope at various magnifications.
• Students should be able to determine types of specimen failure or failed
components. Students are required to identify cause and factors affecting such
failures and give solutions in order to prevent undesirable failures.
• Students can explain influences of forces acting on specimens, microstructures and
test environments on types of fracture modes
• Students should be able to use interpreted data obtained to improve material
properties or to select the right materials for intended applications and to avoid
undesirable failures.
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1. Literature Review
Failures of components in services are undesirable in any engineering applications and should
be avoided in any cases. For example, the failure of the Minnesota Bridge in August 2007, USA has
caused terrible losses in life and required high cost of reconstructions, see figure 1. The cause of the
failure might be plausibly due to insufficient maintenance of the Minnesota Bridge. Failures in aero-
engines, auto parts, or machines during service operations are also undesirable in any cases. In order
to tackle or to avoid any imminent accidents, attempts have been made to understand the causes of
such failures.
Figure 1: Failure of the bridge in Minnesota, USA, August 2007.
Failure analysis deals with studying the causes of failures, analyzing factors influencing
failures and finally solving or preventing such failures that might occur in the future. In order to study
the cause of failure, fractographic observation or fractography has been a powerful tool used for the
determination of failure causes in materials or components. In general, a scanning electron
microscope (SEM) is commonly utilized because it provides a practical range of magnifications
suitable for the investigation. The information obtained from fracture surfaces is used for the analysis
of the failure causes and factors affecting such failures and thus leads to the prevention of failures in
the future. The whole process of failure analysis requires a handful of skills and experiences to come
out with an accurate judgment or corrective preventions. Failure analysis is currently becoming an
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important skill for engineers whose work is relevant to operating machines, components, or
engineering structures.
For a short learning period, this laboratory will provide you the fractographic skills involving
visual inspection, stereo microscope and SEM techniques. These require a good understanding of
different types of fracture in materials. Therefore different fracture modes in metallic materials
should be first introduced here to give you some important background about fractographic
investigation.
1.1 Types of fracture in metals
Types of fracture can be roughly divided into two categories, which are brittle and ductile
fractures. The former has however gained a lot of interests due to its catastrophic results whenever
happens. Limited amount of plastic deformation occurring during brittle fracture, promotes a sudden
failure without warning. Ductile failure on the contrary exhibits rough and dull fracture surfaces with
gross plastic deformation, therefore allowing more time to correct or prevent such failures. This
failure type is not too catastrophic and has gained less interest from many researchers as compared to
brittle failure. Nevertheless, a true understanding of all types of fracture is of importance such that
causes of failure can be accurately determined and can lead to the suitable means of material
selection. Types of fracture are described as follows
• Transgranular fracture, which can be classified into
- Brittle cleavage fracture
- Ductile fracture
- Fatigue fracture
• Intergranular fracture, which can be classified into
- Intergranular fracture without microvoid
- Intergranular fracture with microvoid
1.1.1 Brittle cleavage fracture
Figures 2 (a) and (b) illustrate fractographs of tensile specimens, which have been failed in
ductile and brittle manners respectively. It is noticed in figure 2 (b) that flat surfaces with limited
plastic deformation are belonged to tensile specimens that have been failed in a brittle failure mode.
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Fracture surfaces of the tensile specimen failed in a ductile mode on the other hand exhibit a so called
cup and cone type fracture, showing gross plastic deformation on both half of the fracture surfaces.
Brittle materials normally exhibit flat fracture surfaces consisting of transgranular cleavage
facets. This type of fracture give small areas of fracture surface; hence, requiring low specific surface
energy (γ) to produce two new fresh fracture surfaces. The fracture energy is therefore low in this
case. Figure 2 (b) shows a classic characteristic of brittle facets with their size similar to the grain size
of the material. The brittle facets were caused by a fast propagation of the crack transgranularly
across the grains. Investigated at higher magnifications using a scanning electron microscope (SEM),
the fracture surface show a river line pattern or stress line pattern in which its direction pointing
toward the origin of the crack. A fracture surface of a broken piece of glass might be seen quite
similar to that observed from cleavage fracture. When the crack is initiated possibly at the inclusion,
the metal grains then readily cleave along the low-fracture-energy crystallographic plane. Figure 3 (a)
depicts a transgranular cleavage fracture of ferrite grains in carbon steel. This feature is a true
cleavage fracture. Nevertheless, if some areas of ductile tearing is observed, for example, in the case
of a fracture surface observed in in 17-4 PH stainless steel of a tempered martensite microstructure as
shown in figure 3 (b), this type of fracture surface is called quasi-cleavage fracture [1].
Figure 2 Ductile fracture and brittle cleavage fracture observed from tensile fracture surfaces.
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Figure 3: Fracture surfaces showing (a) cleavage facets of ferrite in carbon steel and b) Quasi
cleavage facets of tempered martensite observed in 17-4 PH stainless steel [1].
The river lines or the stress lines are steps between cleavage or parallel planes, which are
always converged in the direction of local crack propagation as seen from figure 4. This direction is
normally observed pointing to inclusion, porosity, crack or second phase particle, which create stress
concentration. Transgranular cleavage fracture is usually associated with defects such as cracks,
porosity, inclusions or second phase particles in which dislocations movement is obstructed. Stress is
therefore concentrated in front of these defects, initiating a crack of a critical size. The propagation of
this crack then finally causes the global failure with very little plastic deformation as illustrated in
figure 5. As the defects are known as the cause of the failure, minimizing these defects is considered
to avoid stress concentration, hence to increase fracture resistance of the materials. This can be done
by controlling the quality of the products in manufacturing processes.
Figure 4: River line pattern observed from brittle cleavage fracture surfaces [3].
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The crack initiation site can be traced back by studying fracture surfaces of the specimens or
components by visual inspection or by means of using microscopes at different magnifications. An
example of the crack initiation which are obviously observed by naked eyes from fracture surfaces of
metal plates are illustrated in figure 6. There are apparent stress lines pointing to one end of the plate
on both halves as depicted in figure 6 (a) and an initiation site located in the middle of the top surface
as seen in figure 6 (b). However if the identification of sites for crack initiation is not easily carried
out by visual inspection such similar to these cases, SEM investigation is then becoming more
practical. For instance, a fracture surface of a steel fracture toughness specimen was visually
investigated first and the result has shown a possible crack initiation site at point S, according to the
indicating stress lines as demonstrated in figure 5. Investigating at higher magnifications using the
SEM technique reveals areas of cleavage facets with the crack initiated at an inclusion as determined
by the direction of the river line pattern. The inclusion observed was subsequently determined as a
Mg2S particle, which are typically found in steels. Minimizing of these inclusions leads to a
significant improvement in mechanical properties and fracture resistance of the steel.
Figure 5: Fractographic observation indicating initiation site at an inclusion[4].
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Figure 6: Fracture surfaces showing crack initiation sites eventually leading to failures [3].
1.1.2 Ductile fracture
If we now consider a tensile sample which is loaded beyond the maximum tensile strength as
shown in figure 7, we can see necking occurring along the specimen gauge length. Within the
necking area, microvoids are formed probably around the particles. As the load continues, these
microvoids expand and join together to create a crack with its plane perpendicular to the axis of the
tensile force applied. As this crack grows, the shear plane of approximately 45o to the tensile
direction develops around specimen edge and merges with the existing crack, resulting in the classic
cup and cone fracture surfaces as demonstrated in figure 7.
Ductile materials normally exhibit gross plastic deformation during fracture, providing rough
fracture surfaces with relatively high surface areas as has been illustrated in figure 1. Ductile fracture
therefore requires higher energy to create two new fresh fracture surfaces in comparison to energy
required to cleave flat brittle surfaces. Investigation under higher magnifications shows ductile
fracture surface consisting of copious of ductile dimples or microvoids. The mechanism of microvoid
formation is demonstrated in figure 8, showing the influence of inclusions or second phase particles as
microvoid initiation sites. During loading, these particles decohere from the matrix, forming a
microvoid around each particle. Continuing the applied load results in the expansion of these
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microvoids and finally leads to microvoid coalescence, giving the complete failure. Generally, these
microvoids are normally observed to be centred on inclusions or second phase particles as shown in
figure 8 (d). Materials such as ductile cast iron, aluminium or alloys operating at high temperature
exhibit this type of fracture surface.
Figure 7: Cup and cone fracture.
Furthermore, the shape of the microvoids observed in a microscopic scale can be used to
determine the type of the force applied on to the specimen. If the microvoids are in equiaxed shape,
as shown in figure 9 (a), the applied force are uniaxial tensile loading. Parabolic-shaped microvoids
with its tip pointing in the opposite direction when seen on both halves of fracture surface are due to
shear force, see figure 9 (b). If the microvoids appear in the parabolic shape with the tip of each
microvoid orientated in the same direction on both fracture surface halves, the tensile tearing is
applied in this case as shown in figure 9 (c).
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Figure 8: Microvoid coalescence in ductile fracture[4].
Figure 9: Different characteristics of microvoids observed under (a) Uniaxial tensile loading, (b)
shear and (c) tensile tearing[].
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1.1.3 Intergranular fracture
Intergranular fracture is normally associated with service conditions which are corrosive or
high temperature. These conditions resulting in precipitation of the second phase particles along the
weakened grain boundaries. Figure 10 illustrates two types of intergranular fracture; a) intergranular
fracture with microvoid coalescence and b) without microvoid coalescence. Although the former
exhibits areas of ductile dimples similar to those observed from typical ductile fracture surfaces, these
ductile dimples are relatively shallow and require much less energy involved in the fracture process.
These ductile dimples or microvoids are formed around particles precipitated in some cases as a
network along the grain boundaries. This considerably reduces the bonding between the particles and
the matrix, which in turn allows microvoid coalescence to occur more readily. As a result, the
material has significantly reduced fracture energy which promotes a rapid crack propagation path
along the grain boundaries.
Figure 10: Fracture surfaces of (a) Intergranular fracture with microvoid coalescence and (b)
without microvoid coalescence.
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Temperature is one of the most important factors influencing intergranular fracture. High
temperature not only facilitates ductile failure (increased amount of plastic deformation) but also
promotes metallurgical changes. If the bonding between the new phases and the matrix is quite poor,
responses of materials to external loads will be significantly affected, which can subsequently alter the
fracture mode of the materials. In general, oxidation or combustion reactions are involved when
materials are subjected to high temperatures, such as in the case of turbine blades. Oxide scales on the
metal surface are normally brittle and heterogeneously formed, leading to a crack formation on the
surface. If the load continues at high temperature, oxidation would progress even further into material
interior through the existing surface cracks. This might result in the formation of brittle oxidation
products within the grain and especially along the grain boundaries. If these grain boundary oxidation
products are interconnected and poorly bonded with the matrix, intergranular fracture will result.
Therefore, it can be seen that although high temperature promotes ductile failure, metallurgical
changes might alter the fracture mode from transgranular ductile fracture to intergranular fracture due
to poorly bonded grain boundary particles. This embrittlement effect results in noticeable reductions
in tensile strength and ductility. The utilization of the materials at high temperatures or strong
oxidation will considerably affect mechanical properties of the materials. Material selection therefore
becomes significantly important in this case. Nickel based alloys are a good alternative for service
conditions at high temperature and oxidation. Furthermore, material which is subjected to corrosive
environment where corrosion products are observed along the grain boundaries will give comparable
results.
1.1.4 Fatigue fracture
Fatigue fracture surfaces possess quite a unique characteristic of flat surfaces with limited
plastic deformation and in some cases show visible beach mark as shown in the gear teeth subjected to
fatigue failure in figure 12. Surface condition is a prime factor in controlling surface crack initiation.
Crack or defect-free surfaces greatly help to improve fatigue life of the components. Rough surfaces
are also attractive to stress concentration, leading to easy fatigue crack initiation.
In general, initiation and propagation of the fatigue crack can be divided into three stages, 1)
Fatigue crack initiation Bstage I, 2) stable fatigue crack propagation-stage II and 3) Unstable fatigue
crack initiation B stage III. The initiation of the fatigue crack is sensitive to surface conditions.
Figure 12 shows mechanisms of extrusion and intrusion on the top surface of sample subjected to
fatigue loading. Persistent slip planes caused by back and forth motion of fatigue produce a number
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of extrusions and intrusions as illustrated in the schematic diagram. The latter is considered as an
atomic scale notch and acts as a stress raiser to eventually become the initial fatigue crack on such a
surface. The plane of the fatigue crack at this stage is along the shear plane or slip plane. When the
fatigue crack grows a little further, the fatigue crack is now influenced by the tensile stresses which
are perpendicular to the crack propagation direction. The fatigue crack is now said to be in the stage
II region, and propagates at a relatively stable rate. The fatigue propagation rate in this region
therefore represents the fatigue crack growth of the specimen. The final stage is the unstable fatigue
crack propagation which takes place when the fatigue crack length exceeds the critical length for
stable crack growth, leading eventually to fatigue failure.
If we study the stage II fatigue fracture surface using SEM technique, striations orientated
normal to the fatigue crack growth direction as shown in figure 14 (a) will be observed. Each striation
is due to plastic blunting process as demonstrated in figure 14 (b). When the tensile loading
progresses, the crack opens and allows the slips to operate at the top and bottom ends to produce local
plastic deformation as shown by the arrows. At a higher tensile loading, plastic blunting occurs,
which leads to an increase in the fatigue crack length. During unloading, the fatigue crack is then
closed and the slips are now operating in the opposite direction. Therefore, after one cycle, the fatigue
crack now arrives at the original stage of crack closing with an increase in one fatigue striation.
Figure 12: Beach mark observed on a fatigue fracture fracture surface of gear.
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Figure 13: Mechanism of extrusion and intrusion on the top surface due to persistent slip bands [1].
Figure 14: a) Fatigue striations in aluminum and b) Fatigue striation due to plastic blunting process.
Furthermore, the fatigue failure can be found to occur in conjunction with corrosive and high
temperature environment, which are called corrosion fatigue and thermal fatigue respectively.
Corrosion and high temperature accelerate the rate of the fatigue crack propagation and promote
severe fatigue failures. An example of corrosion fatigue shows obvious areas of rust on the fatigue
surface observed in an automobile shaft as depicted in figure 15 (a). This significantly reduces the
fatigue life of the automobile shaft. Thermal fatigue illustrated in figure 15 (b) shows a beach mark
which indicates the fatigue crack initiation to have started at the top surface.
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Figure 15: Fracture surfaces of specimens failed in a) corrosion-fatigue and b) thermal fatigue.
1.2 Fractography techniques
Sample preparation is an important step to ensure accurate information achieved from
fracture surfaces. Failed specimens or components should be kept in an environment that can protect
them from moisture and not to produce oxide scales on the surfaces. Broken halves of fracture
surfaces should not be rubbed against each other. The sample should be cleaned using an ultrasonic
vibration technique and then washed by acetone prior to dry blowing for further investigation.
The techniques and the microscopes used for fractographic investigation come in various
magnifications as schematically shown in figure 16. If the fracture surfaces are too big to put under
any microscopes, visual inspection is very practical and the origin of the failure can be roughly
indicated. Optical microscope and SEM are employed for investigating at higher magnifications to
determine the fracture mode and the crack initiation site on a microscopic scale. Transmission
electron microscope (TEM) is utilized when lattice parameter are required to identify the existing
phases. However sample preparation for TEM technique is a time consuming process and the
interpretation of the acquired data requires adequate understanding.
Figure 16: Equipment used for fractographic observation ranging according to magnification [5].
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The most powerful technique commonly used for fractographic investigation is the SEM
technique. This technique utilizes electron as a source to create images as illustrated in figure 17.
The electron beam released from the electron gun travels pass through the electromagnetic field and
electromagnetic lenses where it is focused prior to hitting on the specimen surface. Then the X-ray,
back scattered electrons, secondary electron and auger electrons are produced. These signals are
subsequently collected to produce images and information important for the interpretation of failure
analysis. Sample preparation for SEM investigation is a critical stage, which requires a proper
cleaning in order to obtain free- moisture surfaces. The sample should also be conductive. However
in the case of non-conductive materials, gold sputtering is normally used to produce conductive
coating on their surfaces. Specimen should be carefully griped onto the specimen holder to avoid
sliding off in the vacuum chamber especially when sample is tilted.
Figure 17: Schematic diagram of SEM operation [Lowa State University].
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2. Experimental procedure
2.1 Broken samples achieved from mechanical tests such as tensile, impact, torsion or fatigue
tests.
2.2 Cleaning equipment (Ultrasonic cleaning equipment)
2.3 Scanning electron microscope coupled with energy dispersive spectroscopy
3. Experimental procedure
3.1 Study the principle of the scanning electron microscope from the skilled operators/technicians
responsible for the machine.
3.2 Examine the fracture surfaces of the broken specimens provided by naked eyes before
gripping them on to a specimen holder and putting it into the chamber. The specimens to be
explored have been failed in brittle cleavage, ductile, intergranular and fatigue failure.
3.3 Examine the specimen surfaces at a low magnification first to locate the sample and then
change to higher magnifications. Determine the nature of each fracture surface such as
phases, facets, dimples etc.
3.4 Sketch the fracture surfaces observed in the table provided and provide descriptions.
3.5 Discuss on the issues such as what type of failure mode of each specimen, which type of
force influencing the failure and factors which might affect the failure. Give conclusions.
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4. Results
Specimen Sketch Description
1
2
3
4
Table 1 Sketches of fracture surfaces of tested specimens.
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Figure 18: Fractographs observed from fractured specimens.
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5. Discussion
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6. Conclusions
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7. Questions
7.1 Describe the characteristics of cleavage facets, microvoids and fatigue striations.
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7.2 Which types of fracture mode do require the most fracture energy? Why?
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7.3 Predict the fracture mode of compacted graphite, aluminium and white cast iron at room
temperature under tensile loading.
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8. References
8.1 Dieter, G.E., Mechanical metallurgy, 1988, SI metric edition, McGraw-Hill, ISBN 0-07-
100406-8.
8.2 Hashemi, S. Foundations of materials science and engineering, 2006, 4th edition, McGraw-
Hill, ISBN 007-125690-3.
8.3 W.D. Callister, Fundamental of materials science and engineering/an interactive e. text,
2001, John Willey & Sons, Inc., New York, ISBN 0-471-39551-x.
8.4 Hull, D., Bacon, D.J., Introduction to dislocations, 2001, Forth edition, Butterworth-
Heinemann, ISBN 0-7506-4681-0.
8.5 Ewaksm H.L., Wanhill, R.J.H., Fracture mechanics, 1986, Edward Arnold, ISBN- 07131
3515 8.