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1
WHEN MATERIALS ARE GETTING
TIRED… Sub-topics
Cyclic stressesFatigueCrack propagationResistance to fatigue
2
FATIGUE: FACTS
Fatigue is important as it is the largest cause of failure in metals, estimated to comprise approximately 90% of all metallic failures; polymers and ceramics are also susceptible to this type of failure.
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FATIGUE FAILURE
Fatigue failures occur due to cyclic loading at
stresses below a material’s yield strength
https://www.youtube.com/watch?v=dGQfUWvP0II
index.html
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SCHEMATIC OF THE STRESS CYCLING ON THE UNDERSIDE OF A WING
Loading cycles can be in the millions for an aircraft;fatigue testing must employ millions of fatigue cyclesto provide meaningful design data.
https://www.youtube.com/watch?v=ywDsB3umK2Y
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FATIGUE Fatigue is a form of failure that occurs in structures
subjected to dynamic and fluctuating stresses Under these circumstances it is possible for failure to
occur at a stress level considerably lower than the tensile or yield strength for a static load.
It is catastrophic and insidious, occurring very suddenly and without warning.
Primary design criterion in rotating parts. Fatigue as a name for the phenomenon based on the
notion of a material becoming “tired”, i.e. failing at less than its nominal strength.
Cyclic strain (stress) leads to fatigue failure. Occurs in metals and polymers but rarely in ceramics. Also an issue for “static” parts, e.g. bridges.
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FATIGUE: GENERAL CHARACTERISTICS
Most applications of structural materials involve cyclic loadinge. Fatigue failure surfaces have three characteristic features:
A (near-)surface defect as the origin of the crack Striations corresponding to slow, intermittent
crack growth Dull, fibrous brittle fracture surface (rapid
growth). Life of structural components generally
limited by cyclic loading, not static strength. Most environmental factors shorten life.
the cracklength exceeds a critical value at theapplied stress.
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THREE STAGES OF FATIGUE First, a tiny crack initiates or nucleates often at a time well
after loading begins. Normally, nucleation sites are located at or near the surface, where the stress is at a maximum, and include surface defects such as scratches or pits, sharp corners due to poor design or manufacture, inclusions, grain boundaries, or dislocation concentrations.
Next, the crack gradually propagates as the load continues to cycle.
Finally, a sudden fracture of the material occurs when the remaining cross-section of the material is too small to support the applied load. Thus, components fail by fatigue because even though the overall applied stress may remain below the yield stress, at a local length scale, the stress intensity exceeds the tensile strength.
For fatigue to occur, at least part of the stress in the material has to be tensile.
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FACTORS CAUSING FATIGUE FAILURE
1) A maximum tensile stress of sufficiently high value.2) A large amount of variation or fluctuation in the applied stress.3) A sufficiently large number of cycles of the applied stress.
• Stress concentration• Corrosion• Temperature• Overload• Metallurgical structure• Residual stress• Combined stress
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CYCLIC STRESSES
Reversed stress cycle, in which thestress alternates from amaximum tensile stressto a maximum compressive stress ofequal magnitude
Repeated stress cycle, in which maximum andminimum stresses areasymmetrical relative tothe zero stress level;mean stress m, range ofstress r , and stressamplitude a are indicated.
Randomstress cycle.
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PARAMETERS
mean stress
range of stress
stress amplitude
stress ratio R
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S-N CURVES S-N [stress-number of cycles to failure] curve
defines number of cycles-to-failure for given cyclic stress.
Rotating-beam fatigue test is standard; also alternating tension-compression.
Plot stress versus the log(number of cycles to failure), log(Nf).
For frequencies < 200Hz, metals are insensitive to frequency; fatigue life in polymers is frequency dependent.
rotating-bending tests
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S–N BEHAVIOR
Stress amplitude (S) versus logarithm of thenumber of cycles tofatigue failure (N) for a material that displays a fatigue limit
The higher the magnitude of the stress, the smaller the number of cycles the material is capable to sustain before failureThere is a limiting stress level, called the fatigue limit (also sometimes the endurance limit), below which fatigue failure will not occur.
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ENDURANCE LIMITS
Some materials exhibit endurance limits, i.e. a stress below which the life is infinite:Steels typically show an endurance limit of
about 40% - 60% of yield strength; this is typically associated with the presence of a solutes (carbon, nitrogen) that pines dislocations and prevents dislocation motion at small displacements or strains.
Aluminum alloys do not show endurance limits; this is related to the absence of dislocation-pinning solutes.
At large Nf, the lifetime is dominated by nucleation. Therefore strengthening the surface (shot penning) is
beneficial to delay crack nucleation and extend life.
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S–N BEHAVIORStress amplitude (S) versus logarithm of the number of cycles tofatigue failure (N) for a material that does not display a fatigue limit.
Most nonferrous alloys (e.g., aluminum, copper, magnesium) do not have a fatigue limit, in that the S–N curve continues its downward trend at increasingly greater N values
Fatigue will ultimately occur regardless of the magnitude of the stress. For these materials, the fatigue response is specified as fatigue strength, which is defined as the stress level at which failure will occur for some specified number of cycles (e.g., 107 cycles).
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FATIGUE LIFEfatigue life Nf
characterizes a material’s fatigue behavior
It is the number of cycles to cause failure at a specified stress level, as taken from the S–N plot
There always exists considerable scatter in fatigue data, that is, a variation in the measured N value for a number of specimens tested at the same stress level. This may lead to significant design uncertainties when fatigue life and/or fatigue limit (or strength) are being considered. The scatter in results is a consequence of the fatigue sensitivity to a number of test and material parameters that are impossible to control precisely. These parameters include specimen fabrication and surface preparation, metallurgical variables, specimen alignment in the apparatus, mean stress, and test frequency.
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STATISTICAL NATURE OF FATIGUE
Because the S-N fatigue data is normally scattered, it should be therefore represented on a probability basis.
Considerable number of specimens is used to obtain statistical parameters.
At σ1, 1% of specimens would be expected to fail at N1 cycles.
50% of specimens would be expected to fail at N2 cycles.
For engineering purposes, it is sufficiently accurate to
assume a logarithmic normal distribution of fatigue life in the region of the probability of failure of P = 0.10 to P = 0.90.
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FATIGUE S–N PROBABILITY OF FAILURE CURVES FOR A 7075-T6 ALUMINUM ALLOY
The probability of failure
The data obtained is normally scattered at the same stress level by using several specimens.This requires statistic approach to define the fatigue limit.
Constant probability
curves
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HIGH- CYCLIC FATIGUE
For low stress levels wherein deformations are totally elastic, longer lives result. This is called high-cycle fatigue inasmuch as relatively large numbers of cycles are required to produce fatigue failure.
High-cycle fatigue is associated with fatigue lives greater than about 104 to 107 cycles.
The S-N curve in the high-cycle region is sometimes described by the Basquin equation
p and C are empirical constants
19
LOW- CYCLE FATIGUE
is associated with relatively high loads that produce not only elastic strain but also some plastic strain during each cycle.
Consequently, fatigue lives are relatively short occurs at less than about 104 to 105 cycles
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DESIGN OF A ROTATING SHAFT A solid shaft for a cement oven produced from
tool steel must be 240 cm long and must survive continuous operation for one year with an applied load of 55,600 N.
The shaft makes one revolution per minute during operation.
Design a shaft that will satisfy these requirements. The
maximum stress acting on this typeof specimen
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PROCESS OF FATIGUE FAILURE
Characterized by three distinct steps: (1) crack initiation, wherein a small crack
forms at some point of high stress concentration;
(2) crack propagation, during which this crack advances incrementally with each stress cycle;
(3) final failure, which occurs very rapidly once the advancing crack has reached a critical size.The fatigue life Nf , the total number of cycles to failure,
therefore can be taken as the sum of the number of cycles for crack initiation Ni and crack propagation Np
The contribution of the final failure step to the total fatigue life is insignificant since it occurs so rapidly
22
CRACK INITIATION
Cracks associated with fatigue failure almost always initiate (or nucleate) on the surface of a component at some point of stress concentration.
Crack nucleation sites include surface scratches, sharp fillets, keyways, threads, dents, and the like.
In addition, cyclic loading can produce microscopic surface discontinuities resulting from dislocation slip steps which may also act as stress raisers, and therefore as crack initiation sites.
23
INITIATION OF FATIGUE CRACK AND SLIPBAND CRACK GROWTH (STAGE I) Fatigue cracks are normally initiated at a free
surface. Slip lines are formed during the first few thousand cycles of stress.
Back and forth fine slip movements of fatigue could build up notches or ridges at the surface => act as stress raiser => initiate crack In stage I, the fatigue crack tends to propagate
initially along slip planes (extrusion and intrusion of persistent slip bands) and later take the direction normal to the maximum tensile stress (stage II).
The crack propagation rate in stage I is generally very low on the order of nm/cycles giving featureless surface.
24
CRACK PROPAGATION Once a stable crack has nucleated, it then initially propagates very slowly and, in polycrystalline metals, along crystallographic planes of high shear stress; this is stage I propagation This stage may constitute a large or small fraction of the total fatigue life depending on stress level and the nature of the test specimen; high stresses and the presence of notches favor a short lived stage I. In polycrystalline metals, cracks normally extend
through only several grains during this propagation stage.
The fatigue surface that is formed during stage I propagation has a flat and featureless appearance
25
FATIGUE CRACK PROPAGATIONMECHANISM
repetitive crack tip plastic blunting and sharpening
zero or maximum compressive load
small tensileload
maximumtensile load
smallcompressive load
zero or maximumcompressive load
small tensile load
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FATIGUE CRACK PROPAGATION
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FATIGUE CRACK PROPAGATIION
For design against fatigue failure, fracture mechanics is utilised to monitor the fatigue crackgrowth rate in the stage II
The fatigue crack growth rate da/dN varies with stress intensity factor range K, which is a function of stress range σ and crack length a.
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STAGE II
ΔK is the stress intensity factor range at the crack tip
Schematicrepresentation of logarithm fatigue crack propagation rate da/dN versus logarithm stress intensity factor range K.
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CRACK PROPAGATION RATE Life of a structural component may be related to
the rate of crack growth. During stage II propagation, cracks may grow
from a barely perceivable size to some critical length. Crack length versus the
number of cycles at stress levels 1 and 2. Crack growth rate da/dN is indicated at crack length a1 for both stress levels.
The parameters A and m are constants for the particular material
30
CRACK GROWTH RATE AND NUMBER OF CYCLES
Knowledge of crack growth rate is of assistance in designing components and in nondestructive evaluation to determine if a crack poses imminent danger to the structure.
Integration between the initial size of a crack and the crack size requiredfor fracture to occur
ai is the initial flaw size and ac is the flaw size required for fracture.
31
DESIGN OF A FATIGUE RESISTANT PLATE A high-strength steel plate, which has a plane
strain fracture toughness of 80 Mpa m1/2 is alternately loaded
in tension to 500 MPa and in compression to 60 MPa. The plate is to survive for 10 years with the stress
being applied at a frequency of once every 5 minutes.
Design a manufacturing and testing procedure that ensures that the component will serve as intended.
• Assume a geometry factor Y = 1.0.
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FORENSIC FRACTURE CASE
• K1c of the tank material measured to be 45 MPa√m• 10 mm crack found in longitudinal weld
Stress based onmaximum design
pressure
Stress at which a plate with the given K1c will fail with a 10 mm crack
HOW LONG IS A LIFE?
How long would it have lasted before fatigue grew the crack to an unstable size?
Residual life = 7 x 106 cycles
34
DESIGN FOR FATIGUE
100 resolutions per second
At least 300 resolutions per second
High-cycle fatigue – 3 x 106 cycles
Selection chart for con-rod based on
material index
Further selectioncriteria includes theuse of S-N curves
For a design life of 2.5 x 106 cycles, a stress of620 MPa can be safely applied
36
FEATURES OF FATIGUE FAILURE two types of markings termed beachmarks
and striations indicate the position of the crack tip at some
point in time and appear as concentric ridges that expand away from the crack initiation site(s), frequently in a circular or semicircular pattern.
Fracture surface of a rotating steel shaft that experienced fatigue failure. Beachmark ridges arevisible in the photograph
37
FACTORS THAT AFFECT FATIGUE LIFE Stress concentration • Size effect • Surface effects • Combined stresses • Cumulative fatigue
damage and sequence effects
• Metallurgical variables
• Corrosion • Temperature
Demonstration of influenceof mean stress m on S–N fatigue behavior
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EFFECT OF MEAN STRESS, STRESS RANGE AND STRESS INTENSITY (NOTCH) ON S-N FATIGUE CURVE
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EFFECT OF STRESS CONCENTRATION ON FATIGUE
Kt is theoretical stress-concentrationfactor, depending on elasticity of crack tipKf is fatigue notch factor, ratio of fatigue strength of notched and unnotchedspecimens
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PROBLEM
Demonstration of how design can reduce stress mplification. (a)Poor design: sharp corner. (b)Good design: fatigue lifetime improved by
incorporating rounded fillet into a rotating shaft at the point where there is a change in diameter.
What design is better?
41
SURFACE EFFECTS ON FATIIGUE
Fatigue properties are very sensitive to surface conditions,
Fatigue initiation normally starts at the surface since the maximum stress is at the surface.
The factors which affect the surface of a fatigue specimen can be roughly divided into three categories
42
SURFACE ROUGHNESS
Different surface finishes produced by different machining processes can appreciably affect fatigue performance.
Polished surface (very fine scratches), normally known as ‘par bar’ which is used in laboratory, gives the best fatigue strength
43
SURFACE RESIDUAL STRESS
Superposition of applied and residual stresses
(a)Shows the elastic stress distribution in a beam with no residual stress.
(b)Typical residual stress distribution produced by shot peening where the high compressive stress is balanced by the tensile stress underneath.
(c) The stress distribution due to the algebraic summation of the external bending stress and the residual stress
Compressive forces on the surface resistcrack growth –
method of producing these stresses is Shot penning
44
COMMERCIAL METHODS INTRODUCINGFAVOURABLE COMPRESSIVE STRESS
Surface rolling - Compressive stress is introduced in between the rollers during sheet rolling
Shot peening - Projecting fine steel or cast-iron shot against the surface at high velocity
Polishing - Reducing surface scratches Thermal stress - Quenching or surface treatments
introduce volume change giving compressive stress.
45
CUMULATIVE FATIIGUE DAMAGE ANDSEQUENCE EFFECTS ON FATIIGUE Practically, levels of stress are not held
constant as in S-N tests, but can vary below or above the designed stress level
Overstressing : The initial applied stress level is higher than the fatigue limit for a short period of time beyond failure, then cyclic stressing below the fatigue limit. This overstressing reduces the fatigue limit.
• Understressing : The initial applied stress level is lower than the fatigue limit for a period of time, then cyclic stressing above the fatigue limit. This understressing increases the fatigue limit (might be due to strain hardening on the surface.
46
EFFECTS OF METALLURGICAL VARIABLLESON FATIGUE
• Fatigue property is normally greatly improved by changing the designs or, reducing stress concentration, introducing compressive stress on the surface.
• Few attempts have paid on improving metallurgical structure to improve fatigue properties but it is still important.
• Fatigue property is frequently correlated with tensile properties.
47
FATIGUE STRENGTH IMPROVEMENT BYCONTROLLING METALLURGICAL VARIABLES
Grain size has its greatesteffect on fatigue life in thelow-stress, high cycle regime
48
FATIGUE STRENGTH IMPROVEMENT BYCONTROLLING METALLURGICAL VARIABLES
• Promote homogeneous slip /plastic deformation through thermo-mechanical processing => reduces residual stress/ stress concentration.
• Heat treatments to give hardened surface but should avoid stress concentration.
• Avoid inclusions = >stress concentration => fatigue strength
• Interstitial atoms increase yield strength , if plus strain aging => fatigue strength
49
EFFECT OF CORROSION ON FATIGUE
Fatigue corrosion occurs when material is subjected to cyclic stress in a corrosive condition.
Corrosive attack produces pitting on metal surface. Pits act as notches => fatigue strength
Chemical attack greatly accelerates the rate of fatigue crack propagation
Corrosion fatigue of brass
Role of a corrosiveenvironment on fatiguecrack propagation
50
THERMAL EFFECT
induced at elevated temperatures by fluctuating thermal stresses;
mechanical stresses from an external source need not be present
The origin of these thermal stresses is the restraint to the dimensional expansion and/or contraction that would normally occur in a structural member with variations in temperature
51
THERMAL FATIGUE Thermal fatigue occurs when metal is subjected to high and low temperature,
producing fluctuating cyclic thermal stress• Normally occurs in hightemperature equipment.• Low thermal conductivity and highthermal expansion properties arecritical.
The thermal stress developed by a temperature change T is
α is linear thermal coefficient of expansionE is elastic modulus
If failure occurs by one application of thermal stress, the condition is called thermal shock.
52
DESIGN FOR FATIGUEThere are several distinct approaches concerning
for design for fatigue 1) Infinite-life design: Keeping the stress at
some fraction of the fatigue limit of the material. 2) Safe-life design: Based on the assumption
that the material has flaws and has finite life. Safety factor is used to compensate for environmental effects, varieties in material production/ manufacturing.
3) Fail-safe design: The fatigue cracks will be detected and repaired before it actually causes failure. For aircraft industry.
4) Damage tolerant design: Use fracture mechanics to determine whether the existing crack will grow large enough to cause failure.
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DESIGN EXAMPLE 1
A relatively large sheet of steel is to be exposed to cyclic tensile and compressive stresses of magnitudes 100 MPa and 50 MPa, respectively. Prior to testing, it has been determined that the length of the largest surface crack is 2.0 mm.
Estimate the fatigue life of this sheet if its plane strain fracture toughness is 25 Mpa m1/2 and the values of m and A are 3.0 and 1.0 x 10-12, respectively, for Δσ in MPa and a in m.
Assume that the parameter Y is independent of crack length and has a value of 1.0.
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