117
Chapter 6 Fatigue Failure Resulting from Variable Loading Tuesday, J une 14, 20 22 Dr. Mohammad Suliman Abuhaiba, PE 1

Chapter 6

Embed Size (px)

DESCRIPTION

Chapter 6. Fatigue Failure Resulting from Variable Loading. Chapter Outline. Introduction to Fatigue in Metals Approach to Fatigue Failure in Analysis and Design Fatigue-Life Methods The Stress-Life Method The Strain-Life Method The Linear-Elastic Fracture Mechanics Method - PowerPoint PPT Presentation

Citation preview

Page 1: Chapter 6

Chapter 6Fatigue Failure Resulting from Variable Loading

Thursday, April 20, 2023

Dr. Mohammad Suliman Abuhaiba, PE1

Page 2: Chapter 6

Chapter Outline

Dr. Mohammad Suliman Abuhaiba, PE

Introduction to Fatigue in Metals Approach to Fatigue Failure in Analysis and Design Fatigue-Life Methods

The Stress-Life Method The Strain-Life Method The Linear-Elastic Fracture Mechanics Method

The Endurance Limit Fatigue Strength Endurance Limit Modifying Factors Stress Concentration and Notch Sensitivity Characterizing Fluctuating Stresses Fatigue Failure Criteria for Fluctuating Stress Torsional Fatigue Strength under Fluctuating Stresses Combinations of Loading Modes Varying, Fluctuating Stresses; Cumulative Fatigue Damage Surface Fatigue Strength Stochastic Analysis Road Maps and Important Design Equations for the Stress-Life Method

Thursday, April 20, 20232

Page 3: Chapter 6

Introduction to Fatigue in Metals

Loading produces stresses that are variable, repeated, alternating, or fluctuating

Maximum stresses well below yield strength

Failure occurs after many stress cyclesFailure is by sudden ultimate fractureNo visible warning in advance of failure

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 20233

Page 4: Chapter 6

Stages of Fatigue Failure

Stage I: Initiation of micro-crack due to cyclic plastic deformation

Stage II: Progresses to macro-crack that repeatedly opens & closes, creating bands called beach marks

Stage III: Crack has propagated far enough that remaining material is insufficient to carry the load, and fails by simple ultimate failure

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 20234

Page 5: Chapter 6

Fatigue Fracture Example

Dr. Mohammad Suliman Abuhaiba, PE

AISI 4320 drive shaft

B: crack initiation at stress concentration in keyway

C: Final brittle failure

Page 6: Chapter 6

Fatigue-Life Methods Three major fatigue life models Methods predict life in number of

cycles to failure, N, for a specific level of loading

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 20236

Page 7: Chapter 6

Fatigue-Life Methods

1. Stress-life method2. Strain-life method3. Linear-elastic fracture

mechanics method

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 20237

Page 8: Chapter 6

1. Stress-Life Method Test specimens subjected to repeated

stress while counting cycles to failure Pure bending with no transverse shear completely reversed stress cycling

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 20238

Page 9: Chapter 6

S-N Diagram

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 20239

Page 10: Chapter 6

S-N Diagram for Steel

Stress levels below Se predict infinite life103 to 106 cycles: finite lifeBelow 103 cycles: low cycle

quasi-static Yielding usually occurs before fatigue

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202310

Page 11: Chapter 6

S-N Diagram for Nonferrous Metals

no endurance limitFatigue strength Sf

S-N diagram for aluminums

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202311

Page 12: Chapter 6

2. Strain-Life Method

Detailed analysis of plastic deformation at localized regions

Compounding of several idealizations leads to significant uncertainties in numerical results

Useful for explaining nature of fatigue

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202312

Page 13: Chapter 6

2. Strain-Life Method Fatigue failure

begins at a local discontinuity

When stress at discontinuity exceeds elastic limit, plastic strain occurs

Cyclic plastic strain can change elastic limit, leading to fatigue

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–12

Thursday, April 20, 202313

Page 14: Chapter 6

Relation of Fatigue Life to Strain

Figure 6–13: relationship of fatigue life to true-strain amplitude

Fatigue ductility coefficient 'F = true strain at which fracture occurs in one reversal (point A in Fig. 6–12)

Fatigue strength coefficient 'F = true stress corresponding to fracture in one reversal (point A in Fig. 6–12)

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202314

Page 15: Chapter 6

Relation of Fatigue Life to Strain

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–13

Thursday, April 20, 202315

Page 16: Chapter 6

Equation of plastic-strain line in Fig. 6–13

Equation of elastic strain line in Fig. 6–13

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202316

Relation of Fatigue Life to Strain

Page 17: Chapter 6

Fatigue ductility exponent c = slope of plastic-strain line

2N stress reversals = N cycles Fatigue strength exponent b = slope

of elastic-strain line

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202317

Relation of Fatigue Life to Strain

Page 18: Chapter 6

Manson-Coffin: relationship between fatigue life and total strain

Table A–23: values of coefficients & exponents

Equation has limited use for design Values for total strain at discontinuities are

not readily availableDr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202318

Relation of Fatigue Life to Strain

Page 19: Chapter 6

The Endurance Limit

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–17

Thursday, April 20, 202319

Page 20: Chapter 6

Simplified estimate of endurance limit for steels for the rotating-beam specimen, S'e

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202320

The Endurance Limit

Page 21: Chapter 6

Fatigue StrengthFor design, an approximation of idealized

S-N diagram is desirable.To estimate fatigue strength at 103

cycles, start with Eq. (6-2)

Define specimen fatigue strength at a specific number of cycles as

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202321

Page 22: Chapter 6

Fatigue StrengthAt 103 cycles,f = fraction of Sut represented by

SAE approximation for steels with HB ≤ 500 may be used.

Dr. Mohammad Suliman Abuhaiba, PE

310( )fS

Thursday, April 20, 202322

Page 23: Chapter 6

Fatigue StrengthTo find b, substitute endurance strength

and corresponding cycles into Eq. (6–9) and solve for b

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202323

Page 24: Chapter 6

Fatigue Strength

Substitute Eqs. 6–11 & 6–12 into Eqs. 6–9 and 6–10 to obtain expressions for S'f and f Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202324

Page 25: Chapter 6

Fatigue Strength Fraction f

Plot Eq. (6–10) for the fatigue strength fraction f of Sut at 103 cycles

Use f from plot for S'f = f Sut at 103 cycles on S-N diagram

Assume Se = S'e= 0.5Sut at 106 cycles

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–18

Thursday, April 20, 202325

Page 26: Chapter 6

Equations for S-N Diagram

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–10

Page 27: Chapter 6

Dr. Mohammad Suliman Abuhaiba, PE

Write equation for S-N line from 103 to 106 cycles Two known points

At N =103 cycles, Sf = f Sut

At N =106 cycles, Sf = Se Equations for line:

Equations for S-N Diagram

Page 28: Chapter 6

Dr. Mohammad Suliman Abuhaiba, PE

If a completely reversed stress rev is given, setting Sf = rev in Eq. (6–13) and solving for N gives,

Typical S-N diagram is only applicable for completely reversed stresses

For other stress situations, a completely reversed stress with the same life expectancy must be used on the S-N diagram

Equations for S-N Diagram

Page 29: Chapter 6

Low-cycle Fatigue 1 ≤ N ≤ 103

On the idealized S-N diagram on a log-log scale, failure is predicted by a straight line between two points (103, f Sut) and (1, Sut)

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202329

Page 30: Chapter 6

Example 6-2

Given a 1050 HR steel, estimatea.the rotating-beam endurance limit at 106 cycles.b.the endurance strength of a polished rotating-beam specimen corresponding to 104 cycles to failurec.the expected life of a polished rotating-beam specimen under a completely reversed stress of 55 kpsi.

Dr. Mohammad Suliman Abuhaiba, PE

Page 31: Chapter 6

Endurance Limit Modifying Factors

Endurance limit S'e is for carefully prepared and tested specimen

If warranted, Se is obtained from testing of actual parts When testing of actual parts is not practical, a set of

Marin factors are used to adjust the endurance limit

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202331

Page 32: Chapter 6

Endurance Limit Modifying Factors

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202332

Page 33: Chapter 6

Surface Factor ka

Surface factor is a function of ultimate strength

Higher strengths are more sensitive to rough surfaces

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202333

Page 34: Chapter 6

Example 6-3A steel has a min ultimate strength of 520 MPa and a machined surface. Estimate ka.

Dr. Mohammad Suliman Abuhaiba, PE

Page 35: Chapter 6

Size Factor kb rotating &

RoundLarger parts have greater surface area

at high stress levelsLikelihood of crack initiation is higher

For bending and torsion loads, the size factor is given by

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202335

Page 36: Chapter 6

Size Factor kb rotating &

RoundApplies only for round, rotating diameterFor axial load, there is no size effect,

kb = 1

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202336

Page 37: Chapter 6

An equivalent round rotating diameter is obtained.

Volume of material stressed at and above 95% of max stress = same volume in rotating-beam specimen.

Lengths cancel, so equate areas.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202337Size Factor kb not round &

rotating

Page 38: Chapter 6

For a rotating round section, the 95% stress area is the area of a ring,

Equate 95% stress area for other conditions to Eq. (6–22) and solve for d as the equivalent round rotating diameter

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202338Size Factor kb not round &

rotating

Page 39: Chapter 6

For non-rotating round,

Equating to Eq. (6-22) and solving for equivalent diameter,

Thursday, April 20, 202339Size Factor kb round & not

rotating

Dr. Mohammad Suliman Abuhaiba, PE

Page 40: Chapter 6

For rectangular section h x b, A95 = 0.05 hb. Equating to Eq. (6–22),

Thursday, April 20, 202340Size Factor kb not round & not

rotating

Dr. Mohammad Suliman Abuhaiba, PE

Page 41: Chapter 6

Size Factor kb

Dr. Mohammad Suliman Abuhaiba, PE

Table 6–3: A95 for common non-rotating structural shapes undergoing bending

Thursday, April 20, 202341

Page 42: Chapter 6

Size Factor kb

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202342

Table 6–3: A95 for common non-rotating structural shapes undergoing bending

Page 43: Chapter 6

Example 6-4

A steel shaft loaded in bending is 32 mm in diameter, abutting a filleted shoulder 38 mm in diameter. The shaft material has a mean ultimate tensile strength of 690 MPa. Estimate the Marin size factor kb if the shaft is used ina.A rotating mode.b.A nonrotating mode.

Dr. Mohammad Suliman Abuhaiba, PE

Page 44: Chapter 6

Loading Factor kc

Accounts for changes in endurance limit for different types of fatigue loading.

Only to be used for single load types. Use Combination Loading method (Sec. 6–14) when

more than one load type is present.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202344

Page 45: Chapter 6

Temperature Factor kd

Endurance limit appears to maintain same relation to ultimate strength for elevated temperatures as at RT

Table 6–4: Effect of Operating Temperature on Tensile Strength of Steel.* (ST = tensile strength at operating temperature (OT); SRT = tensile strength at room temperature; 0.099 ≤ ˆσ ≤ 0.110)

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202345

Page 46: Chapter 6

Temperature Factor kd

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202346

Table 6–4

Page 47: Chapter 6

Temperature Factor kd

If ultimate strength is known for OT, then just use that strength. Let kd = 1.

If ultimate strength is known only at RT, use Table 6–4 to estimate ultimate strength at OT. With that strength, let kd

= 1. Use ultimate strength at RT and apply kd

from Table 6–4 to the endurance limit.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202347

Page 48: Chapter 6

A fourth-order polynomial curve fit of the data of Table 6–4 can be used in place of the table,

Temperature Factor kd

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202348

Page 49: Chapter 6

Example 6-5

A 1035 steel has a tensile strength of 70 kpsi and is to be used for a part that sees 450°F in service. Estimate the Marin temperature modification factor and (Se)450◦ ifa.RT endurance limit by test is (S’e)70◦ = 39.0 kpsib.Only the tensile strength at RT is known.

Dr. Mohammad Suliman Abuhaiba, PE

Page 50: Chapter 6

Reliability Factor ke

Fig. 6–17, S'e = 0.5 Sut is typical of the data and represents 50% reliability.

Reliability factor adjusts to other reliabilities.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202350

Page 51: Chapter 6

Reliability Factor ke

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–17

Thursday, April 20, 202351

Page 52: Chapter 6

Reliability Factor ke

Dr. Mohammad Suliman Abuhaiba, PE

Table 6–5

Thursday, April 20, 202352

Page 53: Chapter 6

Miscellaneous-Effects Factor kf

Consider other possible factors: Residual stresses Directional characteristics from cold working Case hardening Corrosion Surface conditioning

Limited data is available. May require research or testing.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202353

Page 54: Chapter 6

Stress Concentration and Notch Sensitivity Obtain Kt as usual (Appendix A–15)

Kf = fatigue stress-concentration factor q = notch sensitivity, ranging from 0 (not

sensitive) to 1 (fully sensitive)

For q = 0, Kf = 1

For q = 1, Kf = Kt Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202354

Page 55: Chapter 6

Notch SensitivityFig. 6–20: q for bending or axial loading

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–20

Thursday, April 20, 202355

Kf = 1 + q( Kt – 1)

Page 56: Chapter 6

Notch SensitivityFig. 6–21: qs for torsional loading

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202356

Kfs = 1 + qs( Kts – 1)

Page 57: Chapter 6

Notch SensitivityUse curve fit equations for Figs. 6–20 & 6–21 to get notch sensitivity, or go directly to Kf .

Dr. Mohammad Suliman Abuhaiba, PE

Bending or axial:

Torsion:

Thursday, April 20, 202357

Page 58: Chapter 6

Notch Sensitivity for Cast Irons

Cast irons are already full of discontinuities, which are included in the strengths.

Additional notches do not add much additional harm.

Recommended to use q = 0.2 for cast irons.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202358

Page 59: Chapter 6

Example 6-6A steel shaft in bending has an ultimate strength of 690 MPa and a shoulder with a fillet radius of 3 mm connecting a 32-mm diameter with a 38-mm diameter. Estimate Kf using:

a.Figure 6–20b.Equations (6–33) and (6–35)

Dr. Mohammad Suliman Abuhaiba, PE

Page 60: Chapter 6

Application of Fatigue Stress Concentration Factor

Use Kf as a multiplier to increase the nominal stress.

Some designers apply 1/Kf as a Marin factor to reduce Se .

For infinite life, either method is equivalent, since

For finite life, increasing stress is more conservative. Decreasing Se applies more to high cycle than low cycle.

Dr. Mohammad Suliman Abuhaiba, PE

1/ f eef

f

K SSn

K

Thursday, April 20, 202360

Page 61: Chapter 6

Example 6-7

For the step-shaft of Ex. 6–6, it is determined that the fully corrected endurance limit is Se = 280 MPa. Consider the shaft undergoes a fully reversing nominal stress in the fillet of (σrev)nom = 260 MPa. Estimate the number of cycles to failure.

Dr. Mohammad Suliman Abuhaiba, PE

Page 62: Chapter 6

Example 6-8

A 1015 hot-rolled steel bar has been machined to a diameter of 1 in. It is to be placed in reversed axial loading for 70 000 cycles to failure in an operating environment of 550°F. Using ASTM minimum properties, and a reliability of 99%, estimate the endurance limit and fatigue strength at 70 000 cycles.

Dr. Mohammad Suliman Abuhaiba, PE

Page 63: Chapter 6

Example 6-9Figure 6–22a shows a rotating shaft simply supported in ball bearings at A and D and loaded by a non-rotating force F of 6.8 kN. Using ASTM “minimum” strengths, estimate the life of the part.

Dr. Mohammad Suliman Abuhaiba, PEFig. 6–22

Page 64: Chapter 6

Characterizing Fluctuating Stresses

The S-N diagram is applicable for completely reversed stresses

Other fluctuating stresses exist Sinusoidal loading patterns are common, but not necessary

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202364

Page 65: Chapter 6

Fluctuating Stresses

Dr. Mohammad Suliman Abuhaiba, PE

Figure 6–23

fluctuating stress with high frequency ripple

non-sinusoidal fluctuating stress

Page 66: Chapter 6

Fluctuating Stresses

Dr. Mohammad Suliman Abuhaiba, PE

General Fluctuating

Repeated

Completely Reversed

Figure 6–23

Page 67: Chapter 6

Characterizing Fluctuating Stresses

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202367

Stress ratio

Amplitude ratio

Page 68: Chapter 6

Application of Kf for Fluctuating StressesFor fluctuating loads at points with stress

concentration, the best approach is to design to avoid all localized plastic strain.

In this case, Kf should be applied to both alternating and midrange stress components.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202368

Page 69: Chapter 6

Application of Kf for Fluctuating StressesWhen localized strain does occur,

some methods (nominal mean stress method and residual stress method) recommend only applying Kf to the alternating stress.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202369

Page 70: Chapter 6

Application of Kf for Fluctuating StressesDowling method recommends applying

Kf to the alternating stress and Kfm to the mid-range stress, where Kfm is

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202370

Page 71: Chapter 6

Fatigue Failure for Fluctuating Stresses

Vary m and a to learn about the fatigue resistance under fluctuating loading

Three common methods of plotting results follow.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202371

Page 72: Chapter 6

Modified Goodman Diagram

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–24

Thursday, April 20, 202372

Page 73: Chapter 6

Plot of Alternating vs Midrange Stress

Little effect of negative midrange stress

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–25

Thursday, April 20, 202373

Page 74: Chapter 6

Master Fatigue Diagram

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–26

Thursday, April 20, 202374

Page 75: Chapter 6

Plot of Alternating vs Midrange Stress

Most common and simple to use

Goodman or Modified Goodman diagram

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202375

Page 76: Chapter 6

Commonly Used Failure Criteria

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–27

Thursday, April 20, 202376

Page 77: Chapter 6

Modified Goodman is linear, so simple to use for design. It is more conservative than Gerber.

Soderberg provides a very conservative single check of both fatigue and yielding.

Langer line represents standard yield check. It is equivalent to comparing maximum stress to yield strength.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202377Commonly Used Failure Criteria

Page 78: Chapter 6

Equations for Commonly Used Failure Criteria

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202378

Page 79: Chapter 6

Summarizing Tables for Failure Criteria

Tables 6–6 to 6–8: equations for Modified Goodman, Gerber, ASME-elliptic, and Langer failure criteria

1st row: fatigue criterion 2nd row: yield criterion 3rd row: intersection of static and fatigue

criteria 4th row: equation for fatigue factor of safety 1st column: intersecting equations 2nd column: coordinates of the intersectionDr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202379

Page 80: Chapter 6

Dr. Mohammad Suliman Abuhaiba, PE

Table 6–6: Modified Goodman and Langer Failure Criteria (1st Quadrant)

Page 81: Chapter 6

Table 6–7: Gerber & Langer Failure Criteria (1st Quadrant)

Dr. Mohammad Suliman Abuhaiba, PE

Page 82: Chapter 6

Table 6–8: ASME Elliptic and Langer Failure Criteria (1st Quadrant)

Dr. Mohammad Suliman Abuhaiba, PE

Page 83: Chapter 6

Example 6-10A 1.5-in-diameter bar has been machined from an AISI 1050 cold-drawn bar. This part is to withstand a fluctuating tensile load varying from 0 to 16 kip. Because of the ends, and the fillet radius, a fatigue stress-concentration factor Kf is 1.85 for 106 or larger life. Find Sa and Sm and the factor of safety guarding against fatigue and first-cycle yielding, usinga.Gerber fatigue lineb.ASME-elliptic fatigue line.

Dr. Mohammad Suliman Abuhaiba, PE

Page 84: Chapter 6

Example 6-10

Dr. Mohammad Suliman Abuhaiba, PE

Page 85: Chapter 6

Example 6-10

Dr. Mohammad Suliman Abuhaiba, PE

Page 86: Chapter 6

Example 6-11A flat-leaf spring is used to retain an oscillating flat-faced follower in contact with a plate cam. The follower range of motion is 2 in and fixed, so the alternating component of force, bending moment, and stress is fixed, too. The spring is preloaded to adjust to various cam speeds. The preload must be increased to prevent follower float or jump. For lower speeds the preload should be decreased to obtain longer life of cam and follower surfaces. The spring is a steel cantilever 32 in long, 2 in wide, and 1/4 in thick, as seen in Fig. 6–30a. The spring strengths are Sut = 150 kpsi, Sy = 127 kpsi, and Se = 28 kpsi fully corrected. The total cam motion is 2 in. The designer wishes to preload the spring by deflecting it 2 in for low speed and 5 in for high speed.

Dr. Mohammad Suliman Abuhaiba, PE

Page 87: Chapter 6

a. Plot Gerber-Langer failure lines with the load line.

b. What are the strength factors of safety corresponding to 2 in and 5 in preload?

Example 6-11

Dr. Mohammad Suliman Abuhaiba, PE

Page 88: Chapter 6

Example 6-11

Dr. Mohammad Suliman Abuhaiba, PE

Page 89: Chapter 6

Example 6-12A steel bar undergoes cyclic loading such that σmax = 60 kpsi and σmin = −20 kpsi. For the material, Sut = 80 kpsi, Sy = 65 kpsi, a fully corrected endurance limit of Se = 40 kpsi, and f = 0.9. Estimate the number of cycles to a fatigue failure using:a.Modified Goodman criterion.b.Gerber criterion.

Dr. Mohammad Suliman Abuhaiba, PE

Page 90: Chapter 6

Fatigue Criteria for Brittle Materials

First quadrant fatigue failure criteria follows a concave upward Smith-Dolan locus,

Or as a design equation,

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202390

Page 91: Chapter 6

Fatigue Criteria for Brittle Materials

For a radial load line of slope r, the intersection point is

In the second quadrant,

Table A–24: properties of gray cast iron, including endurance limit

Endurance limit already includes ka and kb

Average kc for axial and torsional is 0.9

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202391

Page 92: Chapter 6

Example 6-13A grade 30 gray cast iron is subjected to a load F applied to a 1 by 3/8 -in cross-section link with a 1/4-in-diameter hole drilled in the center as depicted in Fig. 6–31a. The surfaces are machined. In the neighborhood of the hole, what is the factor of safety guarding against failure under the following conditions:The load F = 1000 lbf tensile, steady.The load is 1000 lbf repeatedly applied.The load fluctuates between −1000 lbf and 300 lbf without column action.Use the Smith-Dolan fatigue locus.

Dr. Mohammad Suliman Abuhaiba, PE

Page 93: Chapter 6

Example 6-13

Dr. Mohammad Suliman Abuhaiba, PE

Page 94: Chapter 6

Example 6-13

Dr. Mohammad Suliman Abuhaiba, PE

Page 95: Chapter 6

Torsional Fatigue Strength Testing: steady-stress component has no

effect on the endurance limit for torsional loading if the material is : ductile, polished, notch-free, and cylindrical.

For less than perfect surfaces, the modified Goodman line is more reasonable.

For pure torsion cases, use kc = 0.59 to convert normal endurance strength to shear endurance strength.

For shear ultimate strength, recommended to use

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202395

Page 96: Chapter 6

Combinations of Loading ModesFor combined loading, use Distortion

Energy theory to combine them.Obtain Von Mises stresses for both

midrange and alternating components.Apply appropriate Kf to each type of stress.

For load factor, use kc = 1. The torsional load factor (kc = 0.59) is inherently included in the von Mises equations.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202396

Page 97: Chapter 6

Combinations of Loading ModesIf needed, axial load factor can be

divided into the axial stress.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202397

Page 98: Chapter 6

Static Check for Combination Loading

Distortion Energy theory still applies for check of static yielding

Obtain Von Mises stress for maximum stresses

Stress concentration factors are not necessary to check for yielding at first cycle

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 202398

Page 99: Chapter 6

max a m

Static Check for Combination LoadingAlternate simple check is to obtain

conservative estimate of 'max by summing 'a and 'm

≈Dr. Mohammad Suliman Abuhaiba, PE

1/22 2

max

max

3a m a m

yy

Sn

Thursday, April 20, 202399

Page 100: Chapter 6

Example 6-14A rotating shaft is made of 42×4 mm AISI 1018 CD steel tubing and has a 6-mm-diameter hole drilled transversely through it. Estimate the factor of safety guarding against fatigue and static failures using the Gerber and Langer failure criteria for the following loading conditions:The shaft is subjected to a completely reversed torque of 120 N.m in phase with a completely reversed bending moment of 150 N.m.The shaft is subjected to a pulsating torque fluctuating from 20 to 160 N.m and a steady bending moment of 150 N.m.

Dr. Mohammad Suliman Abuhaiba, PE

Page 101: Chapter 6

Example 6-14

Dr. Mohammad Suliman Abuhaiba, PE

Page 102: Chapter 6

Varying Fluctuating Stresses

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023102

Page 103: Chapter 6

Cumulative Fatigue Damage A common situation is to load at 1 for n1

cycles, then at 2 for n2 cycles, etc. The cycles at each stress level

contributes to the fatigue damage Accumulation of damage is represented

by the Palmgren-Miner cycle-ratio summation rule, also known as Miner’s rule

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023103

Page 104: Chapter 6

Cumulative Fatigue Damage ni = number of cycles at stress level i

Ni = number of cycles to failure at stress level i

c = experimentally found to be in the range 0.7 < c < 2.2, with an average value near unity

D = the accumulated damage,

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023104

Page 105: Chapter 6

Example 6-15Given a part with Sut = 151 kpsi and at the critical location of the part, Se = 67.5 kpsi. For the loading of Fig. 6–33, estimate the number of repetitions of the stress-time block in Fig. 6–33 that can be made before failure.

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–33

Page 106: Chapter 6

Illustration of Miner’s Rule

Figure 6–34: effect of Miner’s rule on endurance limit and fatigue failure line.

Damaged material line is predicted to be parallel to original material line.

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023106

Page 107: Chapter 6

Weaknesses of Miner’s Rule

Miner’s rule fails to agree with experimental results in two ways

1. It predicts the static strength Sut is damaged.

2. It does not account for the order in which the stresses are applied

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023107

Page 108: Chapter 6

Manson’s Method Manson’s method overcomes deficiencies of

Miner’s rule.

Dr. Mohammad Suliman Abuhaiba, PE

Fig. 6–35

Thursday, April 20, 2023108

All fatigue lines on S-N diagram converge to a common point at 0.9Sut at 103 cycles.It requires each line to be constructed in the same historical order in which the stresses occur.

Page 109: Chapter 6

Surface Fatigue StrengthWhen two surfaces roll or roll and slide

against one another, a pitting failure may occur after a certain number of cycles.

The surface fatigue mechanism is complex and not definitively understood.

Factors include Hertz stresses, number of cycles, surface finish, hardness, lubrication, and temperature

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023109

Page 110: Chapter 6

From Eqs. (3–73) and (3–74), the pressure in contacting cylinders,

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023110

Surface Fatigue Strength

Page 111: Chapter 6

Converting to radius r and width w instead of length l,

pmax = surface endurance strength (contact strength, contact fatigue strength, or Hertzian endurance strength)

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023111

Surface Fatigue Strength

Page 112: Chapter 6

Surface Fatigue StrengthCombining Eqs. (6–61) and (6–63),

K1 = Buckingham’s load-stress factor, or wear factor

In gear studies, a similar factor is used,

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023112

Page 113: Chapter 6

Surface Fatigue StrengthFrom Eq. (6–64), with material property

terms incorporated into an elastic coefficient CP

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023113

Page 114: Chapter 6

Surface Fatigue StrengthExperiments show the following

relationships

Data on induction-hardened steel give (SC)10

7 = 271 kpsi and (SC)108 = 239

kpsi, so β, from Eq. (6–67), is

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023114

Page 115: Chapter 6

Surface Fatigue StrengthA long standing correlation in steels

between SC and HB at 108 cycles is

AGMA uses

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023115

Page 116: Chapter 6

Surface Fatigue StrengthIncorporating design factor into Eq. (6–

66),

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023116

Page 117: Chapter 6

Surface Fatigue StrengthSince this is nonlinear in its stress-load

transformation, the definition of nd depends on whether load or stress is the primary consideration for failure.

If loss of function is focused on the load,

If loss of function is focused on the stress,

Dr. Mohammad Suliman Abuhaiba, PE

Thursday, April 20, 2023117