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7/22/2019 Fatigue Failure Resulting From Variable Loading (1)
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F a t i g u e F a i l u r e R e s u l t i n gf r o m Va r i a b l e L o a d i n g
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Variable Loading Variable loading results when the applied load or
the induced stress on a component is not constantbut changes with time
In reality most mechanical components experience
variable loading due to-Change in the magnitude of applied load
Example: Extrusion process
-Change in direction of load applicationExample: a connecting rod
-Change in point of load application
Example: a rotating shaft
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Fatigue
Fatigue is a phenomenon associated with variable
loading or more precisely to cyclic stressing orstraining of a material
ASTM Definition of fatigue
The process of progressive localized permanent
structural changes occurring in a material subjected
to conditions that produce fluctuating stresses at
some point or points and that may result in cracks or
complete fracture after a sufficient number of
fluctuations.
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Fracture Failure- Mechanism
Three stages are involved in fatigue failure
-Crack initiation-Crack propagation
-Fracture / Rupture
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Fracture Failure- Mechanism
Crack propagation modes.
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fatigue failure of the crankshaft under pure bending load.
Fatigue failure
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Crack initiation, propagation and rupture in a shaft subjected to repeated bending
Introduction to Fatigue in Metals
Crack initiation at
the outer surface
Beach marks
showing the nature
of crack propagation
Final rupture occurs
over a limited area,
characterizing a very
small load required
to cause it
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Crack initiation at the root of
keyway at B
Final failure over the smallarea at C due to sudden
rupture
Crack propagation occurs
over a time period
Introduction to Fatigue in Metals
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Connecting rod failed by fatigue failure
The crack got initiated at the flash line of forging.
Flash line of
forging
Introduction to Fatigue in Metals
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Fatigue failure of a steam engine connecting rod due to PURE TENSION load.
No surface crack.
Crack may initiate
anywhere that is the
weakest or unknown
source of weakness.
In this rod, the crack
initiated due to forging
flake slightly below the
centre line.The crack propagated radially outward
until some time after which the sudden
rupture occurred.
Radial direction of
crack propagation
Introduction to Fatigue in Metals
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Approach to Fatigue Failure in Analysis and Design
Fatigue life methods
Fatigue strength and endurance limit
Endurance limit modifying factors
Stress concentration and notch sensitivity Fluctuating stresses
Combination of loading modes
Variable, fluctuating stresses, cumulative fatigue
damage
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Fatigue Life Methods
predict the failure in number of cycles N to failure for a specific type of loading
33 10:(HCF)fatiguecycleHigh;101:(LCF)fatiguecycleLow > NN Stress life methods
Based on stress levels only
Least accurate of the three, particularly for LCF
It is the most traditional because easiest to implement for a wide range of applications
Has ample supporting data
Represents high cycle fatigue adequately Strain life methods
Involves more detailed analysis of plastic deformation at localized regions
Good for LCF
Some uncertainties may exist in results because several idealizations get compounded
Hence normally not used in regular practice but only for completeness and special occasions
Linear elastic fracture mechanics methods (LEFM) Assumes that crack is already present and detected
The crack location is then employed to predict crack growth and sudden rupture with respect tothe stress nature and intensity
Most practical when applied to large structures in conjunction with computer codes and periodicinspection
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Stress Life Method
R. R. Moore high-speed rotating
beam machine.
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pure reversed bending without transverse shear
SFD
BMD
Mb
Stress Life Method
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Stress Life Method
Pure bending by means of weights and no transverse shear.
The specimen shown is very carefully machined and polished witha final polishing in the axial direction to void circumferential
scratches.
Number of revolutions of the specimen required for failure arerecorded.
The first test is made at a stress that is some what under the
ultimate strength of the material.
Next, the test is repeated for a lower load, and so on.
The results are plotted in the S-N diagram, which is either semi-log
or log-log.
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The S-N Diagram for steel (UNS G41300), normalized, Sut=812 MPa.
Endurance Limit,
It is the stress at which the
component can sustain
infinite number of cycles
Stress Life Method: S-N Diagram
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The plot in the S-N diagram never becomes horizontal
for non-ferrous metals and alloys For non-ferrous metals and alloys, stress at a specific
number of cycles, normally at 5*108 cycles, must be
used as fatigue strength
Endurance limit for non-ferrous metals and alloys
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For different aluminium alloys (which is non-ferrous)
For non-ferrous metals and alloys, the S-N diagram never becomes horizontal and
hence they do not have endurance limit. Therefore, a stress at a specific number
of cycles, normally at 5*108 cycles, must be used as fatigue strength
Stress Life Method: S-N Diagram
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Instead of referring to experimental data-bank each time,it should be possible to quickly estimate the value ofendurance limit using some kind of formula
To enable that, data has been generated for differenttypes of steels, for endurance limit with respect to the
ultimate tensile strength This plot seemed to closely follow a combination of two
straight lines, of which the second being almost
horizontal at Sut=1460 MPa
Estimation of Endurance Limit
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Estimation of Endurance Limit
For steels, Endurance limit :
conditionsloadingactualin thelimitEndurance
bendingreverseinobtainedlimitEndurance
1460700
146050
'
'
=
=
>
=
e
e
ut
utut
e
S
S
MPaSforMPa
MPaSforS.S
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Endurance limit (Se) is only for rotational bending of
round bar at idealistic conditions (prepared very
carefully and tested under closely controlled conditions).
Endurance strength (Se) is for all other types of loading,geometry and operating conditions.
Endurance limit Vs. Endurance strength
Endurance limit Endurance strength
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Endurance limit modifying factors'
eedcbae SkkkkkS =
strengthendurancei.e.useofconditionandgeometry
theinpartmachineaoflocationcriticalat thelimitenduranceS
limitendurancespecimentestbeam-otaryS
factoronmodificatim
factorr
factoronmodificati
factoronmodificatiload
factoronmodificatisize
factoronmodificaticonditionsurface
e
'
e
=
=
=
=
=
=
=
=
r
effectsusiscellaneok
eliabilityk
etemperaturk
k
k
k
f
e
d
c
b
a
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b
uta aSk =
Table 6.2; page:288
Surface condition modification factor (ka)
The surface modification factor depends on the quality of the finish of
the actual part surface and on the tensile strength of the part material.
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Size modification factor, kb
( )
1.effect,sizenoloadingaxialFor
25451000837.0859.0
5179.224.162.7/
:onlytorsionandendinginarsCScircularrotatingFor
107.0107.0
=
==
b
b
k
mmdifd
mmdifddk
etc.sectioncrosschannelsection,-Ir,rectangulacircular,
butrotating-nonarethatbarsaboutWhat
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( )[ ]
dd
dA
dddA
Case
e
eee
37.0(2)and(1)Equation
),2(01046.0
i.e0.95dofspacingahavingchordsparalleltwoof
outsideareathetwiceisareastresspercent95the
rounds,solidgnonrotatinFor
),1(0766.095.04
circularrotatingfor:1
2
95.0
222
95.0
=
=
==
K
K
Kb for non-rotating shapes
Effective dimension is used
Effective dimension de obtained by equating the volume of
material stressed at and above 95 percent of the maximum stressto the same volume in the rotating-beam specimen
Table 6-3; page:290
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Load modification factor, kc
=torsion
axial
bending
kc
,59.0
,85.0
,1
Actually the kc is dependent on
the Sutof the material. Tables 6-
11 to 6-14 (page no. 333) in
Text Book give the details. Theabove values are average
values.
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Temperature modifying factor, kd
When operating temperatures are below room
temperature, brittle fracture is a strong possibility andshould be investigated first.
When the operating temperatures are higher than room
temperature, yielding should be investigated first becausethe yield strength drops off so rapidly with temperature.
Any stress will induce creep in a material operating at
high temperatures
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Temperature modifying factor, kd
FT
where
TTTTk
o
F
FFFFd
100070
10595.010104.010115.010432.0975.041238253
++=
145 tests of 21 different carbon and alloy steels results a
fourth-order polynomial curve fit to the data underlying
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Temperature modifying factor, kd( ) ( ) ( ) ( )
FT
where
TTTTk
o
F
FFFFd
100070
10595.010104.010115.010432.0975.0 41238253
++=
Effect of Operating Temperature on the Tensile Strength of Steel.(ST= tensile strength at operating temperature;SRT= tensile strength at room temperature)
Table 6.4; page :291
RT
Td
S
Sk =
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ae zk 08.01=
Reliability factor, ke
Table 65
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Accounts for
Residual stress due to shot-peening, hammering
etc.
Corrosion
Coating failure
Spraying etc.
Miscellaneous effects factor, kf
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Estimate the endurance strength of the given material for the following two cases
1. A32 mm diameter shaft made of hot rolled AISI 1040 steel. The shaft surfaces are grinded. The shaft is
subjected to reverse torque and to be used for a part that sees 250C in service at 99.99% reliability.
2. A solid 20 mm side-square rod is cantilevered at one end. The rod supports a completely reverse axial load at
the other end. The material is AISI 1015 cold-drawn steel. The expected reliability of the rod is 90%.
Problem
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Two steels are being considered for manufacture of forged
connecting rods. One is AISI 4340 Cr-Mo-Ni steel capable of
being heat-treated to a tensile strength of 1820 MPa. The otheris a plain carbon steel AISI 1040 with an attainable Sut of 790
MPa. If each rod is to have a size giving an equivalent diameter
of 20 mm, is there any advantage to using the alloy steel for this
fatigue application?
Problem
For 4340 Cr-Mo-Ni steel, Sut = 1820 MPa For 1040 HR steel, Sut = 790 MPa
899.0)20(24.124.1107.0107.0 === dkb
155.0)1820(272
995.0
===
b
uta Sak 385.0)730(272995.0
===
b
uta Sak
.1;1;1;899.0 ==== edcb kkkk.1;1;1 === edc kkk
MPaSe 54.97)700()1()1()1()899.0()155.0( == MPaSe 75.136)395()1()1()1()899.0()385.0( ==
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The single most influential factor leading to high
possibility of crack initiation
Stress concentration can be due to
Function of geometry (sudden change in
size/diameter; holes in the structure etc.and surface texture (surface finish, presence of
disintegrations etc.)
Stress concentration
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Kt=Theoretical stress concentration factor
Stress concentration (Kt)-revised
stressNominal
stressMaximum=tK
( )
FEMassuchsimulationnumerical
orsexperimentthroughDetermined
stressNominal
max
=
=
=
t
nomt
K
K
tdwP
dw
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Kf is a reduced value ofKt and it is also called as fatigue
strength reduction factor
Actual / Fatigue stress concentration factor, Kf
factor)(geometricfactorionconcentratstresslTheoretica
21)-6&20-6Fig.(fromy valuesensitivitnotch
=
=
tK
q
( ) ( )1111 +=+= tsshearfstf KqKorKqK
specimenfree-notchinstress
specimennotchedinstressmaximum=fK
Stress-concentration factors for a variety of geometries under different
loading conditions can be found in Table A15 (page:1026-1032)
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Notch Sensitivity plot for Steels and UNS A92024-T wrought Al alloys
Fig: 6-20 ; page : 295
(Reverse bending or reverse axial loads)
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Notch Sensitivity plot for Steels and UNS A92024-T wrought Al alloys
(Reversed torsion condition)
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Estimation of KfKf= 1+q(Kt -1).
When q=0, the material has no sensitivity to notches, and henceKf=1.
When q=1, or when notch radius is large for which q is almost equal
to 1, the material has full notch sensitivity, andKf=Kt.
For all grades of cast iron, use q=0.20.Use the different graphs as given to obtain q for bending/axial and
torsional loading.
Whenever the graphs do not give values ofq for certain combinationsof data, use eitherNeuber equation orHeywood equation.
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Use theNeuber equation when the notch is circular/cylindrical.Estimation of Kf
( )
radiusnotchstrength.ultimateoffunctioni.e),(
constantmaterialaisandconstantNeuberisawhere
11
1
1
==
+=
+
=
rSfa
KqKand
ra
q
ut
tf
For steel, withSutin kpsi, the Neuber constant can be approximated
by a third-orderpolynomial fit of data as
38253
38253
)10(67.2)10(35.1)10(51.219.0:
)10(67.2)10(51.1)10(08.3246.0:
ututut
ututut
SSSaTorsion
SSSaaxialorBending
+=
+=
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Use Heywood equation when the notch is NOT circular/cylindrical
but is a tranverse hole or shoulder or groove.
Estimation of Kf
( )
335page15;-6Tabletheingivenarevalues
121
a
where
r
a
K
K
KK
t
t
tf
+
=
r= hole/ shoulder/groove size
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Fluctuating Stress
2
stresseor variablamplitude
2stressmeanormidrange
stressofrange
stressmaximumstressminimum
minmax
minmax
minmax
max
min
==
+==
==
==
a
m
r
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Reversed: mean stress is zero;equal reversals on both sides;
useful in conducting experiments
Repeated: minimum stress is zero;mean stress equal to half of therange stress
Fluctuating: maximum, minimumand mean stress are all non-zeroand arbitrary
Three specific types of cyclic loading:
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Design for Infinite life under cyclic loading
fyt
m
e
a
nSS
1=+
1=+yt
m
e
a
S
S
S
S
1=+ut
m
e
a
S
S
S
S
1
2
=
+
ut
m
e
a
S
S
S
1
22
=
+
yt
m
e
a
S
S
S
S
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Different fatigue failure models
yielding)staticfor
checkingfor(onlylineLanger1
lineEllipticASME1
lineGerber1
lineGoodmanModified1
lineSoderberg1
222
2
K
K
K
K
K
yyt
m
yt
a
fyt
m
e
a
fut
m
fe
a
fut
m
e
a
fyt
m
e
a
nSS
nSS
nSn
S
nSS
nSS
=+
=
+
=
+
=+
=+
Where aofamofm KandK ==
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Modified Goodman and
Langer Failure Criteria
Amplitude and Steady Coordinates of Strength and Important
Intersections in First Quadrant
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Gerber and Langer
Failure Criteria
Amplitude and Steady Coordinates of Strength and Important
Intersections in First Quadrant
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ASME-Elliptic and Langer
Failure Criteria
Amplitude and Steady Coordinates of Strength and Important
Intersections in First Quadrant
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Results based on Smiths tests (72 tests on torsion
strength) and confirmation by Joerres of AssociatedSpring-Barnes Group, the following relation is
used to identify the shear ultimate strength from
tensile strength.
From distortion energy theory,
utsu S0.67S =
ytsy S0.577S =
Torsional Fatigue Strength
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An AISI 1020 cold drawn steel shaft of diameter 30
mm is welded to a fixed support at one end and
another end is subjected to a bending moment
varying from 25 Nm to 100 Nm. Fatigue stress
concentration factor under bending (Kf) is 1.6. Findthe factor of safety using the Gerber failure criteria.
Problem:
390470S;SteelCD1020AISIFor MPaSandMPa ==
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( )( )
( )( )
.
38.61
470
73.37
196.8
64.22
1SS
equation;failurefatigueGerber
MPa196.8=Skkk=S
1=k
0.95830)1.24(0.37=)1.24(d=k
drawn)coldfor-0.265=band4.51=(a0.874=aS=k
MPa235=0.5S=S
64.2215.146.1
73.3758.236.115.14
58.23
43.930
10253232
72.3730
101003232
390470S;SteelCD1020AISIFor
2
2
ut
m
e
a
1
ecbae
c
0.107-0.107-
eb
b
uta
ut
1
e
3
3
3
min
3
3
3
max
ut
safetyfactorhighwithdesignedoverismemberThe
nn
n
nn
MPaK
MPaKMPastressbendingVariable
MPastressbendingMean
MPad
MstressbendingMinimum
MPad
M
stressbendingMaximum
MPaSandMPa
f
f
f
f
f
bafa
bmfm
ba
bm
y
==
+
=
+
=
===
=====
==
=
==
=
==
==
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Different types of cyclic loads may be applied incombination, for example, bending, axial and torsional
on machine components
When the loads and in-phase, the maximum values ofloads occurs at the same time and so are the minimum
values.
Hence in such cases, we can estimate the maximum andminimum von-Mises stress values and then estimate the
mean and amplitude von-Mises stresses. Then fatiguecriterion may be applied.
Combination of loading modes
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Combined loadingFor the common case of a shaft with bending stresses, torsional shear
stresses, and axial stresses, the von Mises stress is
Considering that the bending, torsional, and axial stresses have
alternating and midrange components, the von Mises stresses for the
two stress elements can be written as
For plane stress
[ ]21
222' 3 xyyyxx ++=[ ]2
122' 3 xyx +=
( ) ( ) ( )
( )
( ) ( )[ ]( ) ( ) ( ) ( )[ ] ( ) ( )[ ]{ } 2/122'
2/1
2
2
'
3
385.0
torsionmotorsionfsaxialmoaxialfbendingmobendingfm
torsionaotorsionfs
axialao
axialfbendingaobendingfa
KKK
KKK
++=
+
+=
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Calculate von Mises stresses for alternating and
midrange stress states, a and m .
Apply stresses to fatigue criterion i.e Soderberg,
Modified-Goodman, Gerbers or ASME Elliptic criteria
by replacing a and m with a and m respectively
Conservative check for localized yielding using von
Mises stresses i.e
Design for Combined loading
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Fig shows clutch-testing machine. The steel shaft rotates at a constant speed
. An axial load is applied to the shaft and is cycled from zero to P. The
torque T induced by the clutch face onto the shaft
where D and d are defined in the figure and f is the coefficient of friction of
the clutch face. The shaft is machined with Sy = 800 MPa and Sut = 1000
MPa. The theoretical stress concentration factors for the fillet are 3.0 and 1.8for the axial and torsional loading, respectively.
Assume the load variation P is synchronous
with shaft rotation. With f = 0.3, find themaximum allowable load P such that the shaft
will survive a minimum of 108 cycles with a
factor of safety of 3. Use the modified
Goodman criterion.
Prob:6-57
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Solution
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Solution
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Practice problemIn the figure shaft A, made of AISI 1010 hot-rolled steel, is welded to afixed support and is subjected to loading by equal and opposite forces F via
shaft B. In addition, the shaft is also subjected to a study compressive force
of P. The length of shaft A from the fixed support to the connection at shaftB is 1 m. If the load F cycles from 0.5 to 2kN and P= 1 kN, For shaft A find
the factor of safety for infinite life using (a) the modified Goodman fatigue
failure criterion. (b) Gerber fatigue failure criterion.
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Strain-Life method is used to estimate fatigue
strength for high cycle fatigue (i.e. N>103 cycles)
Fatigue strength
If a completely reversed stress(rev
) in given, the
number of cycles to failure can be expressed as
( )
==
=
e
ut
e
ut
b
f
SfSb
SfSa
whereNaS
log31&
2
Fatigue strength calculation / Design for finite life
brev
a
N
1
=
Where f is fatigue strengthfraction depends on Sut from
Figure 6-18; page:285
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Fatigue strength fraction
Figure 6-18; page:285
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A 25-mm-diameter solid round bar has a groove 2.5-mm
deep with a 2.5-mm radius machined into it. The bar is
made of AISI 1020 CD steel and is subjected to a purely
reversing torque of 200 N-m. For the S-N curve of this
material, letf= 0.9.
(a) Estimate the number of cycles to failure.
(b) If the bar is also placed in an environment with a
temperature of 4500F, estimate the number of cycles to
failure.
Problem : 6-12
Solution
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D= 25 mm ; d= 20 mm ; r= 2.5 mm
r/d =2.5/20 = 0.125; D/d= 1.25From figure: Kts= 1.4
Solution
Sol tion
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MPaSandkpsiMPa y 390)68(470S;SteelCD1020AISIFor ut ==
Solution
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( )
cyclesa
N
S
fSb
S
fSa
MPa
ba
se
su
se
su
22472
169.0log3
1
94.913
315S0.67S
MPa87.94=Skkk=S
0.59=k0.7260)21.24(=)1.24(d=k
drawn)coldfor-0.265=band4.51=(a0.874=aS=k
MPa235=0.5S=S
1
2utsu
1
ecbae
c
0.107-0.107-
eb
b
uta
ut
1
e
=
=
=
=
==
==
=
Solution
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