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    MECH 401

    Mechanical Design Applications

    Dr. M. OMalleyMaster Notes

    Spring 2008

    Dr. D. M. McStravickRice University

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    Reading

    Chapter 6

    Homework

    HW 4 available, due 2-7

    Tests

    Fundamentals Exam will be in class on 2-21

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    Nature of fatigue failure

    Starts with a crack

    Usually at a stress concentration

    Crack propagates until the material fractures

    suddenly

    Fatigue failure is typically sudden and

    complete, and doesnt give warning

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    Fatigue Failure Examples

    Various Fatigue Crack Surfaces [Text fig. 6-2]

    Bolt Fatigue Failure [Text fig. 6-1]

    Drive Shaft [Text fig. 6-3]

    AISI 8640 Pin [Text fig. 6-4]

    Steam Hammer Piston Rod [Text fig. 6-6] Jacob Neu chair failure (in this classroom)

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    Fatigue Example 1

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    Fatigue Failure Example

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    Fatigue Failure Example

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    Fatigue Failure Example

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    Stamping Fatigue Failure Example

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    Schematic of Various Fatigue Failure

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    Fatigue Failure of Chair Shaft

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    Seat Fatigue Failure

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    Fatigue

    Fatigue strength and endurance limit

    Estimating FS and EL

    Modifying factors

    Thus far weve studied static failure of machine elements

    The second major class of component failure is due to dynamic loading Variable stresses

    Repeated stresses

    Alternating stresses

    Fluctuating stresses

    The ultimate strength of a material (Su) is the maximum stress a

    material can sustain before failure assuming the load is applied onlyonce and held

    A material can also fail by being loaded repeatedly to a stress level thatis LESS than Su Fatigue failure

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    More Fatigue Failure Examples (ASM)

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    More Fatigue Failure Examples (ASM)

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    More Fatigue Failure Examples

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    The 3 major methods

    Stress-life Based on stress levels only

    Least accurate for low-cycle fatigue

    Most traditional Easiest to implement

    Ample supporting data

    Represents high-cycle applications adequately Strain-life

    More detailed analysis of plastic deformation at localized regions

    Good for low-cycle fatigue applications

    Some uncertainties exist in the results

    Linear-elastic fracture mechanics

    Assumes crack is already present and detected Predicts crack growth with respect to stress intensity

    Practical when applied to large structures in conjunction with computercodes and periodic inspection

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    Fatigue analysis

    2 primary classifications of

    fatigue

    Alternatingno DC component

    Fluctuatingnon-zero DC

    component

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    Analysis of alternating stresses

    As the number of cyclesincreases, the fatigue strengthSf(the point of failure due tofatigue loading) decreases

    For steel and titanium, thisfatigue strength is never lessthan the endurance limit, Se

    Our design criteria is:

    As the number of cyclesapproaches infinity (N ),Sf(N) = Se (for iron or Steel)

    a

    f NS

    )(

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    Method of calculating fatigue strength

    Seems like we should be able to use graphslike this to calculate our fatigue strength ifwe know the material and the number ofcycles

    We could use our factor of safety equationas our design equation

    But there are a couple of problems with thisapproach S-N information is difficult to obtain and thus is

    much more scarce than -einformation

    S-N diagram is created for a lab specimen Smooth

    Circular

    Ideal conditions Therefore, we need analytical methods for

    estimating Sf(N) and Se

    a

    f NS

    )(

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    Estimating Se Steel and Iron

    For steels and irons, we can estimate the

    endurance limit (Se) based on the ultimate

    strength of the material (Sut)

    Steel Se = 0.5 Sut for Sut< 200ksi (1400MPa)

    = 100ksi (700MPa) for all other values of Sut

    Iron Se = 0.4(min Sut)f/ gray cast Iron Sut

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    S-N Plot with Endurance Limit

    a

    eS

    a

    f NS

    )(

    a

    eS

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    Estimating Se Aluminum and Copper

    Alloys For aluminum and copper alloys, there is no endurance limit

    Eventually, these materials will fail due to repeated loading

    To come up with an equivalent endurance limit, designerstypically use the value of the fatigue strength (Sf) at 10

    8cycles

    Aluminum alloys

    Se (Sfat 108cycles) = 0.4 Sut for Sut< 48 ksi (330 MPa)

    = 19 ksi (130 MPa) for all other values of Sut

    Copper alloys

    Se (Sfat 108cycles) = 0.4 Sut for Sut< 35 ksi (250 MPa)= 14 ksi (100 MPa) for all other values of Sut

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    Constructing an estimated S-N diagram

    Note that Se is going to be ourmaterial strength due to infiniteloading

    We can estimate an S-N diagramand see the difference in fatiguestrength after repeated loading

    For steel and iron, note that thefatigue strength (Sf) is never lessthan the endurance limit (Se)

    For aluminum and copper, notethat the fatigue strength (S

    f)

    eventually goes to zero (failure!),but we will use the value of Sfat108cycles as our endurance limit(Se) for these materials

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    Estimating the value of Sf

    When we are studying a case offatigue with a known number of cycles(N), we need to calculate the fatiguestrength (Sf)

    We have two S-N diagrams

    One for steel and iron One for aluminum and copper

    We will use these diagrams to comeup with equations for calculating Sffor a known number of cycles

    Note: Book indicates that 0.9 is notactually a constant, and uses thevariable fto donate this multiplier.We will in general use 0.9 [so f=0.9]

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    Estimating Sf(N)

    For steel and iron

    For f=0.9

    For aluminum and copper

    bSa

    S

    Sb

    aNNS

    ut

    e

    ut

    b

    f

    39.0loglog

    9.0log

    3

    1

    '

    -

    -

    bSa

    SSb

    aNNS

    ut

    e

    ut

    b

    f

    39.0loglog

    9.0log31

    '

    -

    -

    For 103< N < 106

    For N < 108

    Where Se is the value ofSfat N = 10

    8

    5.7

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    Correction factors

    Now we have Se (infinite life)

    We need to account for differences between the lab specimen and a realspecimen (material, manufacturing, environment, design)

    We use correction factors Strength reduction factors

    Marin modification factors

    These will account for differences between an ideal lab specimen and real life

    Se= kakbkckdkekfSe kasurface factor

    kbsize factor

    kcload factor

    kdtemperature factor

    kereliability factor

    Kfmiscellaneous-effects factor

    Modification factors have been found empirically and are described in section 6-9 ofShigley-Mischke-Budynas (see examples)

    If calculating fatigue strength for finite life, (Sf), use equations on previous slide

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    Endurance limit modifying factors

    Surface (ka) Accounts for different surface finishes

    Ground, machined, cold-drawn, hot-rolled, as-forged

    Size (kb) Different factors depending on loading

    Bending and torsion (see pg. 280)

    Axial (kb= 1)

    Loading (kc) Endurance limits differ with Sutbased on fatigue loading (bending, axial, torsion)

    Temperature (kd) Accounts for effects of operating temperature (Not significant factor for T

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    Surface Finish Effect on Se

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    Temperature Effect on Se

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    Reliability Factor, ke

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    Compressive Residual Stresses

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    Now what?

    Now that we know the strength of our part under

    non-laboratory conditions

    how do we use it?

    Choose a failure criterion Predict failure

    Part will fail if:

    > Sf(N)

    Factor of safety or Life of the part:

    = Sf(N) /

    Where

    b = - 1/3 log (0.9 Sut/ Se) log (a) = log (0.9 Sut) - 3b

    b

    aN

    1

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    Example Homework Problem 6-9

    A solid rod cantilevered at one end. The rod is

    0.8 m long and supports a completelyreversing transverse load at the other end of +/-1 kN. The material is AISI 1045 hot-rolledsteel. If the rod must support this load for 104

    cycles with a factor of safety of 1.5, whatdimension should the square cross sectionhave? Neglect any stress concentrations at thesupport end and assume f= 0.9.

    Solution: -- See Board Work--

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    Stress concentration (SC) and fatigue failure

    Unlike with static loading, both ductile and

    brittle materials are significantly affected by

    stress concentrations for repeated loading

    cases We use stress concentration factors to modify

    the nominal stress

    SC factor is different for ductile and brittlematerials

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    SC factorfatigue

    = kfnom+ =kfo

    t= kfstnom = kfsto

    kfis a reduced value of kTand ois the nominalstress.

    kfcalled fatigue stress concentration factor

    Why reduced? Some materials are not fully sensitiveto the presence of notches (SCs) therefore,depending on the material, we reduce the effect ofthe SC

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    Fatigue SC factor

    kf= [1 + q(kt1)]

    kfs= [1 + qshear(kts1)] ktor kts and nominal stresses

    Table A-15 & 16 (pages 1006-1013 in Appendix)

    q and qshear Notch sensitivity factor

    Find using figures 6-20and 6-21in book (Shigley) for steelsand aluminums

    Use q = 0.20 for cast iron

    Brittle materials have low sensitivity to notches

    As kfapproaches kt, q increasing (sensitivity to notches, SCs)

    If kf~ 1, insensitive (q = 0)

    Property of the material

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    Example, cont.

    = Se/

    What do we need?

    Se

    Considerations? Infinite life, steel

    Modification factors

    Stress concentration (hole)

    Find nom(without SC)

    F

    F

    hdb

    P

    A

    Pnom 2083

    101260

    -

    -

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    Example, cont.

    Now add SC factor:

    From Fig. 6-20,

    r = 6 mm

    Sut= 448 MPa = 65.0 ksi

    q ~ 0.8

    nomtnomf kqk - 11

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    Example, cont.

    From Fig. A-15-1, Unloaded hole

    d/b = 12/60 = 0.2

    kt~ 2.5

    q = 0.8

    kt= 2.5

    nom= 2083 F

    F

    Fkq nomt

    4583

    208315.28.0111

    --

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    Example, cont.

    Now, estimate Se Steel:

    Se = 0.5 Sutfor Sut< 1400 MPa (eqn. 6-8)

    700 MPa else AISI 1020 As-rolled

    Sut= 448 MPa

    Se = 0.50(448) = 224MPa

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    Constructing an estimated S-N diagram

    Note that Se is going to be ourmaterial strength due to infiniteloading

    We can estimate an S-N diagramand see the difference in fatiguestrength after repeated loading

    For steel and iron, note that thefatigue strength (Sf) is never lessthan the endurance limit (Se)

    For aluminum and copper, notethat the fatigue strength (Sf)

    eventually goes to zero (failure!),but we will use the value of Sfat108cycles as our endurance limit(Se) for these materials

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    Correction factors

    Now we have Se (infinite life)

    We need to account for differences between the lab specimen and a realspecimen (material, manufacturing, environment, design)

    We use correction factors Strength reduction factors

    Marin modification factors

    These will account for differences between an ideal lab specimen and real life

    Se= kakbkckdkekfSe kasurface factor

    kbsize factor

    kcload factor

    kdtemperature factor

    kereliability factor

    Kfmiscellaneous-effects factor

    Modification factors have been found empirically and are described in section 6-9 ofShigley-Mischke-Budynas (see examples)

    If calculating fatigue strength for finite life, (Sf), use equations on previous slide

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    Example, cont.

    Modification factors

    Surface: ka= aSutb(Eq. 6-19)

    a and b from Table 6-2

    Machined

    ka= (4.45)(448)-0.265= 0.88

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    Example, cont.

    Size: kb

    Axial loading

    kb= 1 (Eq. 6-21)

    Load: kc Axial loading

    kc= 0.85 (Eq. 6-26)

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    Example, cont.

    Temperature: kd= 1 (no info given)

    Reliability: ke= 1 (no info given)

    Miscellaneous: kf= 1

    Endurance limit: Se= kakbkckdkekfSe = (0.88)(0.85)(227) = 177 MPa

    Design Equation:

    kN4.21

    8.14583

    10x177

    8.14583177

    6

    F

    FMPaSe

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    Fluctuating Fatigue Failures

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    Alternating vs. fluctuating

    Alternating Fluctuating

    I

    Mr

    A

    P

    a

    m

    Al

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    Alternating Stresses

    acharacterizes alternating stress

    Fl i

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    Fluctuating stresses

    Mean Stress

    Stress amplitude

    Together, m

    and a

    characterize fluctuating

    stress

    2' minmax

    m

    2

    minmax'

    -a

    Al i Fl i

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    Alternating vs. Fluctuating

    M difi d G d Di

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    Modified Goodman Diagram

    Fl i S i C i d

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    Fluctuating Stresses in Compression and

    Tension

    F il i i f fl i l di

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    Failure criterion for fluctuating loading

    Soderberg Modified Goodman

    Gerber

    ASME-elliptic

    Yielding

    Points above the line: failure

    Book uses Goodman primarily

    Straight line, therefore easy algebra

    Easily graphed, every time, for every problem Reveals subtleties of insight into fatigue problems

    Answers can be scaled from the diagrams as a check on thealgebra

    G b L Pl f Fl i S

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    Gerber Langer Plot for Fluctuating Stresses

    Fl i

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    Fluctuating stresses, cont.

    As with alternating stresses, fluctuating stresses have beeninvestigated in an empirical manner

    For m< 0 (compressive mean stress) a> Sf Failure

    Same as with alternating stresses

    Or,

    Static Failure

    For m> 0 (tensile mean stress) Modified Goodman criteria

    < 1 Failure

    )S(ormax ucycam S-

    1ut

    m

    f

    a

    SS

    M difi d G d L E i

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    Modified Goodman Langer Equations

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    S i l f fl t ti t

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    Special cases of fluctuating stresses

    Case 1: mfixed

    Case 2: afixed

    a

    aS

    m

    mS

    S i l f fl t ti t

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    Special cases of fluctuating stresses

    Case 3: a/ mfixed

    Case 4: both vary arbitrarily

    m

    m

    a

    a SS

    ut

    m

    f

    a

    SS

    1

    E l

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    Example

    Given:

    Sut= 1400 MPa

    Syt= 950 MPa

    Heat-treated (as-forged)

    Fmean= 9.36 kN

    Fmax= 10.67 kN

    d/w = 0.133; d/h = 0.55

    Find:

    for infinite life, assuming

    Fmeanis constant

    E pl t

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    Example, cont.

    Find mand a

    MPa28

    MPa228

    MPa200

    Nm8003.0100.67x14

    1

    4

    1

    22

    Nm7023.010x36.941

    41

    22

    m009.02

    mx1016.318107512

    1

    12

    1

    12

    1

    max

    maxmaxmax

    max

    3

    maxmax

    max

    3

    max

    48333

    -

    --

    -

    ma

    mm

    mm

    m

    I

    yMI

    yM

    LFLF

    M

    LFLFM

    hy

    hdwbhI

    I

    My

    Str C tr ti F t r

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    Stress Concentration Factor

    E mple ont

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    Example, cont.

    Since this is uniaxialloading,

    m= 200 MPa

    a= 28 MPa

    We need to take care ofthe SC factors

    Su = 1400Mpa

    kt~ 2.2 (Figure A15-2) q ~ 0.95 (Figure7-20)

    kf= 2.14

    11 - tf kqk

    nominal

    MPa42820014.2

    MPa602814.2

    nom

    nom

    mfmm

    afaa

    k

    k

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    Example cont

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    Example, cont.

    Design criteria Goodman line:

    For arbitrary variation in

    aand m,

    nSS ut

    m

    e

    a /1

    121

    1400

    11400121

    ma

    25.1

    1400

    428

    121

    601

    1

    1400121

    ma

    Example cont

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    Example, cont.

    However, we know thatFmean= constant from

    problem statement

    m= constant

    4.160

    84

    MPa84

    11400

    428

    121

    1

    a

    a

    a

    a

    ut

    m

    e

    a

    S

    S

    S

    SS

    S

    Less conservative!

    Combined loading and fatigue

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    Combined loading and fatigue Size factor depends on loading

    SC factors also depend on loading

    Could be very complicated calculation to keep track of each loadcase

    Assuming all stress components are completely reversing andare always in time phase with each other,1. For the strength, use the fully corrected endurance limit for

    bending, Se

    2. Apply the appropriate fatigue SC factors to the torsional stress,the bending stress, and the axial stress components

    3. Multiply any alternating axial stress components by the factor1/kc,ax

    4. Enter the resultant stresses into a Mohrs circle analysis to findthe principal stresses

    5. Using the results of step 4, find the von Mises alternating stressa

    6. Compare a with Sato find the factor of safety

    Additional details are in Section 6-14

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