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Chapter 6: Fatigue Failure (Review)I)II)III)IV)V)VI)Sec 6-17 Road Maps and Important EquationsLoadingSimple loading- Axial loading- Torsion- BendingCombined LoadingCharacterizing Stress (Fig. 6-23d, e, f)Completely reversed stressRepeated stressFluctuating stressEndurance Limit 𝑺′𝒆 (Eq. 6-8)Correction Factors: π’Œπ’‚ π’Œπ’ƒ π’Œπ’„ π’Œπ’… π’Œπ’† (Sec. 6-9)Corrected Endurance Limit 𝑺𝒆 (Sec. 6-18)Equivalent StressesTheoretical stress concentration factors: π’Œπ’• π’Œπ’•π’” (A-15)North sensitivity: 𝒒 𝒒𝒔𝒉𝒆𝒂𝒓 (Sec. 6-10)Fatigue stress concentration factors: π’Œπ’‡ π’Œπ’‡π’” (Eq. 6-32)Von Mises Stress for alternating comp. (Eq. 6-55)Von Mises Stress for mid-range comp. (Eq. 6-56)πˆβ€²π’Ž 𝟎 (𝑺𝒆𝒄. πŸ” πŸ–)If πˆβ€²π’‚ 𝑺𝒆 ; infinite life and factor of safety is:𝑺𝒆𝒏 β€²πˆπ’‚Else finite life and number of stress cycles 𝑡 is by (Eq. 6-16) where πˆπ’“π’†π’— is set to πˆβ€²π’‚πˆβ€²π’Ž 𝟎 (𝑺𝒆𝒄. πŸ” 𝟏𝟐)Decide what to use, Soderberg? Modified Goodman? Gerber? ASME Elliptic?(Eq. 6-45 to Eq. 6-48) for factor of safety 𝒏.If 𝒏 𝟏, finite life.Else finite life and 𝑡 is by (Eq. 6-16) but πˆπ’“π’†π’— is per Step 4 on pp. 340.

Figure 1: Fluctuating StressFigure 2: Repeated StressFigure 3: Completely Reversed Stress

Example (1): A low carbon steel stock is lathe-turned to have a diameter of 1” The stock has 𝑆𝑒𝑑 100 π‘˜π‘ π‘–, 𝑆𝑦 76 π‘˜π‘ π‘–. Axial load varies 10 50 π‘˜π‘–π‘π‘ . Fatigue stress concentration factor is 𝐾𝑓 1.3.Find factor of safety 𝑛 if infinite life, or number of cycles 𝑁 if infinite life. Assume room temperature and99% reliability.Case: Simple loading, fluctuating stressπΉπ‘šπ‘–π‘› 10 π‘˜π‘–π‘π‘ πΉπ‘šπ‘Žπ‘₯ 50 π‘˜π‘–π‘π‘ π‘˜π‘“ πΉπ‘šπ‘–π‘› 16.552 π‘˜π‘ π‘–π΄π‘˜π‘“ πΉπ‘šπ‘Žπ‘₯ 82.761 π‘˜π‘ π‘–π΄πœŽπ‘šπ‘–π‘› πœŽπ‘šπ‘Žπ‘₯πœŽπ‘š 33.105 π‘˜π‘ π‘–πœŽπ‘Ž 49.657 π‘˜π‘ π‘–π‘†π‘’β€² 0.5𝑆𝑒𝑑 50 π‘˜π‘ π‘–π‘˜π‘Ž 0.797π‘˜π‘ 1π‘˜π‘ 0.85π‘˜π‘‘ 1π‘˜π‘’ 0.814𝑆𝑒 27.572 π‘˜π‘ π‘–CriterionSoderbergModified GoodmanGerberASME-elliptic 𝑓𝑖𝑛𝑖𝑑𝑒 470.540.54πœŽπ‘Ÿπ‘’π‘£ , οΏ½οΏ½ 0.845π‘Ž 258.97 π‘˜π‘ π‘–π‘ 0.16213CriterionSoderbergModified GoodmanGerberASME-elliptic(see pp. 314 for procedure)

Chapter 7: Shafts and Shaft ComponentsPart 1(7-1): Introduction(7-2): Shaft Materials(7-4): Design for StressPart 2(7-5): Deflection Calculations(7-6): Critical Speeds for ShaftsPart 3(7-3): Shaft Layout(7-7): Misc. Shaft Components(7-8): Limits and Fits(7-1): IntroductionShaft Loading Power transmission shafting is to transmit power/motion from an input source (e.g. motors,engines) to an output work site. Shafts are supported by bearings, and loaded torsionally, transversely, and/or axially as themachine operates. Shafts can be solid or hollow, and are often stepped. They are widely required by virtually all types of machinery and mechanical systems.New Shaft Design Procedure Conceptual sketch for shaft layout, based on functional spec. and system config (7-3) Shaft materials (7-2) An appropriate design factor Support reactions, bending moment diagrams (in tow planes, as well as resultant/combined),and torque diagram, critical cross-sections. Shaft diameters based on strength requirement (7-4) Slopes and Deflections at locations of interest in order to select bearings, couplings, etc.: or toensure proper functioning of bearings, couplings, gears, etc. (7-5) Critical Speeds and other vibration characteristics (7-6)Calculations Needed Shaft diameters based on strength requirement by ANSI/ASME standard B106-1M-1985β€œDesign for Transmission Shafting”, or by other practices. Slopes and deflections simplified / approximate geometry, numerical, graphical, FEA; Critical speed and other vibration characteristics specific deflections of shaft.(7-2): Shaft Materials Requiring generally/typically high strength and high modulus of elasticity Typical selection: low carbon steel (cold-drawn or hot-rolled) such as ANSI 1020-1050 steels If higher strength is required, alloy steels plus heat treatment such as ANSI 1340-50, 4140, 4340,5140, 8650.

Cold-drawn steel is used for diameters under 3 inches; machining is not needed where there isno fitting with other components.Hot-rolled steels should be machined all over.Stainless steels when environment is corrosive, for example.Equations for the Fatigue Failure Criteria(6-40) Soderbeg(6-41) Modified Goodman(6-42) Gerber(6-43) ASME-EllipticFor factor of safety:Replace π‘†π‘Ž with π‘›πœŽπ‘ŽReplace π‘†π‘š with π‘›πœŽπ‘šResulting in Equations (6 45) (6 48)For πœŽπ‘Ÿπ‘’π‘£ (which is needed for number of cycles 𝑁):Replace π‘†π‘Ž with πœŽπ‘ŽReplace π‘†π‘š with πœŽπ‘šReplace 𝑆𝑒 with πœŽπ‘Ÿπ‘’π‘£and solving for πœŽπ‘Ÿπ‘’π‘£Modified-Goodman line – too dangerous, goes directly to 𝑆𝑒𝑑Soderberg – too conservativeMost of the time, we’ll be using ASME-elliptic line, notExample (2): A non-rotating shaft is lathe-turned to have a 1”-diameter. The shaft is subject to a torquethat varies 0 π‘‡π‘šπ‘Žπ‘₯ (𝑖𝑛 𝑙𝑏 𝑖𝑛). Determine π‘‡π‘šπ‘Žπ‘₯ such that the shaft will have an infinite life with afactor of safety of 1.8. The shaft’s material has 𝑆𝑒𝑑 100 π‘˜π‘ π‘– and 𝑆𝑦 76 π‘˜π‘ π‘–. Assume roomtemperature and 99% reliability. Fatigue stress concentration factor is π‘˜π‘“π‘  1.6.

Answer: Based on simple loading and ASME-elliptic criterion, π‘‡π‘šπ‘Žπ‘₯ 2480 𝑙𝑏 𝑖𝑛Design Factor vs. Factor of Safety (not from the text) Design factor is to indicate the level of overload that the part/component is required/intended towithstand Safety factor indicated how much overload the designed part will actually be able to withstand. Design factor is chosen, generally in advance and often set by regulatory code or an industry’sgeneral practice. Safety factor is obtained from design calculations.The following are some recommended values of design factor based on strength considerations. Theyare valid for general applications. 1.25 - 1.5: for reliable materials under controlled conditions subjected to loads and stresses knownwith certainty;1.5 – 2: for well-known materials under reasonably constant environmental conditions subjected toknown loads and stresses;2 – 2.5: for average materials subjected to known loads and stresses;2.5 – 3: for less well-known materials under average conditions of load, stress and environment;3 – 4: for untried materials under average conditions of load, stress and environment;3 – 4: for well-known materials under uncertain conditions of load, stress and environment.Courtesy of Mechanical Design, 2nd Edition, P. Childs, Elsevier Ltd. (p. 95)(7-4): Shaft Design for StressLoads on a Shaft The primary function of a shaft is to transmit torque, typically through only a portion of the shaft; Due to the means of torque transmission, shafts are subject to transverse loads in two planes suchthat the shear and bending moment diagrams are needed in two planes.Shaft Stress from Fatigue Perspective In 1985, ASME published ANSI/ASME Standard B106.1M-1985 β€œDesign for Transmission Shafting”.However, it was withdrawn in 1994.o Little or no axial loado Fully reversed bending and steady (or constant) torsion General case: Fluctuating bending and fluctuating torsiono As considered by the textFully reversed bending and steady torsion is in fact special cases of the general one. In reality, thegeneral case is not as common as the typical case of fully reversed bending and steady torsion.Critical LocationsStresses are evaluated at the critical locations. Look or where: Bending moment is largeThere is torqueThere is stress concentration

Factor of Safety or Required Shaft Diameter – General CaseGenerally, πœŽπ‘π‘’π‘›π‘‘π‘–π‘›π‘” πœŽπ‘š and πœŽπ‘ŽAnd πœπ‘‘π‘œπ‘Ÿπ‘ π‘–π‘œπ‘› πœπ‘š and πœπ‘ŽAssuming negligible axial load, due to fluctuating bending and fluctuating torsion, the amplitude andmean stresses are given by (Eq. 7-1) and (Eq. 7-2):For solid shaft, stresses can be written in terms of 𝑑, the diameter, see (Eq. 7-3) and (Eq. 7-4):Next, the equivalent (von Mises) amplitude and mean stresses are determined, resulting in (Eq. 7-5) and(Eq. 7-6):Now, define terms A and B (pp. 361):Finally, the pair of equations determining factor of safety and diameter, are (DE stands for distortionenergy): For DE-Goodman: (Eq. 7-7), (Eq. 7-8)

For DE-Gerber: (Eq. 7-9), (Eq-7-10) For DE-ASME-Elliptic: (Eq. 7-11), (Eq. 7-12) For DE-Soderberg: (Eq. 7-13), (Eq. 7-14)

After the above fatigue-based calculations, it is customary to check against static failure. The factor of safety against yielding in the first loading cycle is (Eq. 7-16):β€²Where the equivalent maximum stress is πœŽπ‘šπ‘Žπ‘₯by (Eq. 7-15) A quick but conservative check against yielding in the first loading cycle is, see the paragraphfollowing (Eq. 7-16):𝑛𝑦 πœŽπ‘Žβ€²π‘†π‘¦β€² πœŽπ‘šFactor of Safety or Required Shaft Diameter – Typical CasesThe typical case is defined as, fully reversed bending and steady (or constant) torsion. Therefore, settingπ‘€π‘š 0 and π‘‡π‘Ž 0 in above equations will result in what are needed.ASME-Elliptic:Setting π‘€π‘š 0 and π‘‡π‘Ž 0, (Eq. 7-5) and (Eq. 7-6) and the A and B terms become:πœŽπ‘Žβ€² πœŽπ‘Ž2 (𝐾𝑓32π‘€π‘Ž 2 𝐾𝑓 32π‘€π‘Ž) 𝑛𝑑3𝑛𝑑3

β€²πœŽπ‘š 3𝐾𝑓𝑠 16π‘‡π‘šπ‘›π‘‘ 3𝐴 2𝐾𝑓 π‘€π‘Žπ΅ 3𝐾𝑓𝑠 π‘‡π‘š(Eq. 7-11) and (Eq. 7-12) become,1𝑛 2πœŽβ€²πœŽβ€² ( π‘Ž ) ( π‘š )𝑆𝑒𝑆𝑦2𝑛𝑑 3161𝐴 2𝐡 2 ( ) ( )𝑆𝑒𝑆𝑦216𝐴 2𝐡 𝑑 ( ) ( )3𝑛𝑑𝑆𝑒𝑆𝑦3And (Eq. 7-15) simplified to:β€²πœŽπ‘šπ‘Žπ‘₯ 16 𝐴2 𝐡2𝑛𝑑3Estimating 𝑺𝒆 Shaft design equations involve 𝑆𝑒 which in turn involves five modification factors. Therefore, it requires knowing the material, its surface condition, the size and geometry (stressraisers), and the level of reliability. Material and surface condition can be decided before the analysis. The sizes and geometry are however unknown in the preliminary stage of design. For size factor, a diameter may be determined from safety against yielding, or use 0.9 as theestimate of size factor. Reliability is typically set at 90%. Stress concentration factors 𝐾𝑑 and 𝐾𝑑𝑠 for first iteration are given in (Table 7-1, pp. 365)After that (For values not in table - second round), we would have to use (A-15)

Example 7-1Loading and design details are given. We are asked to, (1) determine 𝑛 using DE-Goodman, DE-Gerber,DE-ASME, and DE-Soderberg; and (2) check against yielding failure by evaluating 𝑛𝑦Example 7-2Countershaft AB carries two spur gears at G and J; is supported by two bearings at A and B. Its layout isshown in Figure 7-10. Gear loads areπ‘Ÿπ‘Š23 197 π‘™π‘π‘‘π‘Š23 540 π‘™π‘π‘Ÿπ‘Š54 885 π‘™π‘π‘‘π‘Š54 2431 𝑙𝑏We are to select appropriate materials and/or diameters at various cross sections, based on fatigue withinfinite life. Design factor is 1.5.The text starts with cross-section 𝐼 where there are torque and bending moment, and a shoulder forstress concentration. Generous shoulder fillet (r/d 0.1) is assumed DE-Goodman is used to determinediameters.ExampleA critical cross-section of a shat is subject to a combined bending moment of 63-lb-in and a torque of 74lb-in. The cross-section is the seat of a rolling-element bearing, and sharp shoulder fillet is expected.Shaft material is SAE 1040 CD. Estimate the shaft’s diameter at the cross-section for infinite life with𝑛? 1.5. Base calculations on ASME-Elliptic criterion. Operating conditions are typical.

Solution(1) First iterationπ‘€π‘Ž 63 𝑙𝑏 π‘–π‘›π‘‡π‘š 74 𝑙𝑏 𝑖𝑛𝑆𝑒𝑑 85 π‘˜π‘ π‘–π‘†π‘¦ 71 π‘˜π‘ π‘–π‘†π‘’β€² 42.5 π‘˜π‘ π‘–π‘˜π‘Ž 2.7(85) 0.265 0.832π‘˜π‘ 0.9π‘˜π‘ 1π‘˜π‘‘ 1π‘˜π‘’ 0.897𝑆𝑒 28.55 π‘˜π‘ π‘–π‘˜π‘‘ 2.7π‘˜π‘‘π‘  2.2Set π‘ž π‘žπ‘ β„Žπ‘’π‘Žπ‘Ÿ 1, so that 𝐾𝑓 𝐾𝑑 2.7 and 𝐾𝑓𝑠 𝐾𝑑𝑠 2.2, and𝐴 2𝐾𝑓 π‘€π‘Ž 340.2 𝑙𝑏 𝑖𝑛𝐡 3𝐾𝑓𝑠 π‘‡π‘š 282.0 𝑙𝑏 𝑖𝑛216𝑛𝐴 2𝐡 𝑑 ( ) ( ) 0.458"πœ‹π‘†π‘’π‘†π‘¦3Round off 𝑑 12 π‘šπ‘š 0.472"(2) Second iterationπ‘€π‘Ž 63 𝑙𝑏 π‘–π‘›π‘‡π‘š 74 𝑙𝑏 𝑖𝑛𝑆𝑒𝑑 85 π‘˜π‘ π‘–π‘†π‘¦ 71 π‘˜π‘ π‘–π‘†π‘’β€² 42.5 π‘˜π‘ π‘–π‘˜π‘Ž 2.7(85) 0.265 0.832π‘˜π‘ 0.879(0.472) 0.107 0.953π‘˜π‘ 1π‘˜π‘‘ 1π‘˜π‘’ 0.897𝑆𝑒 30.23 π‘˜π‘ π‘–π‘Ÿπ‘‘ 0.02, then π‘Ÿ 0.009” , and π‘ž 0.57, π‘žπ‘ β„Žπ‘’π‘Žπ‘Ÿ 0.6, so that 𝐾𝑓 1.91 and𝐾𝑓𝑠 1.66Finally,𝐴 2𝐾𝑓 π‘€π‘Ž 240.7 𝑙𝑏 𝑖𝑛𝐡 3𝐾𝑓𝑠 π‘‡π‘š 212.8 𝑙𝑏 𝑖𝑛

πœ‹π‘‘31𝑛 ()( 2.41622𝐴𝐡 ( ) ( )𝑆𝑒𝑆𝑦16 𝐴2 𝐡2 15.56 π‘˜π‘ π‘–πœ‹π‘‘3𝑆𝑦𝑛𝑦 β€² 4.6πœŽπ‘šπ‘Žπ‘₯β€²πœŽπ‘šπ‘Žπ‘₯ Therefore, 𝑑 12 π‘šπ‘š or 0.472" is sufficient, giving a factor of safety against fatigue at 2.4 and a factorof safety against yielding at 4.6.(7-5) Deflection ConsiderationWhy deflection considerations? Shaft deflects transversely like a beam. Shaft also has torsional deflection like a torsion bar. Excessive deflections affect the proper functioning of gears and bearings, for example. Permissibleslopes and transverse deflections are listed in Table 7-2. To minimize deflections, keep shaft short, and avoid cantilever or overhang.How to Determine Beam Deflection AnalyticallyClosed-form solutions (4-4)Superposition (4-5)Singularity Functions (4-6)Strain Energy (4-7)Castigliano’s 2nd Theorem (4-8)Statically indeterminate beams (4-10) .and so on.Limitations: effective when EI const. (but a stepped shaft does not have constant I) Numerical integrationSimplified geometry; for example, small shoulders (diameter-wise and length-wise), fillets, keyways,notches, etc., can be omitted.May be tedious.

ExampleA stepped shaft is shown below, which is supported by ball bearings at A and F. Determine its maximum(in magnitude) lateral deflection, and the slopes at A and F. Use 𝐸 30 𝑀𝑝𝑠𝑖.1) Plot bending moment 𝑀(π‘₯)2) Plot 𝑀/𝑑464𝑀 (πœ‹πΈ ) 𝑀 π‘˜π‘€/𝑑4𝐸𝐼𝑑43) Integrate𝑀 "π‘ π‘™π‘œπ‘π‘’"𝑑44) Integrate "π‘ π‘™π‘œπ‘π‘’"𝑀 "π‘‘π‘’π‘“π‘™π‘’π‘π‘‘π‘–π‘œπ‘›"𝑑45) Baseline6) Deflection7) Slope

To obtain deflection curve of step (6), at any cross-section, subtract value obtained in step (4) frombaseline value.For example, at B, step (4) has 5107.0;baseline value is 26,123; 21,106 26,123 5107.0 will be used in step (6)

117,552 lb/inπ‘ π‘™π‘œπ‘π‘’ π‘œπ‘“ π‘π‘Žπ‘ π‘’π‘™π‘–π‘›π‘’ π‘š 117,552 𝑙𝑏( ) 3265.3 𝑙𝑏/𝑖𝑛236"𝑖𝑛7) Subtract the slope of the baseline from value obtained in step (3)

64𝑖𝑛2 0.6791 10 6 ( )πœ‹πΈπ‘™π‘π‘™π‘π‘–π‘›2 π›Ώπ‘šπ‘Žπ‘₯ (26,113 ) (0.679 10 6)𝑖𝑛𝑙𝑏 0.0177 𝑖𝑛 𝑙𝑏𝑖𝑛2πœƒπ΄ (3265.3 2 ) (0.679 10 6)𝑖𝑛𝑙𝑏 0.00222 π‘Ÿπ‘Žπ‘‘ 𝑇𝑂𝐷𝑂 π‘π‘’π‘Ÿπ‘£π‘’πœƒπΉ 0.00181 π‘Ÿπ‘Žπ‘‘ 𝑇𝑂𝐷𝑂 π‘π‘’π‘Ÿπ‘£π‘’π‘˜ Comments regarding the numerical integration method:Applicable to simple supports as outlined;Fixed supports?More divisions for better accuracy;Vertical plane, horizontal plane, and vector sum.An exact numerical method for determining the bending deflection and slope of stepped shafts, C.R.Mischke, in Advanced in reliability and stress analysis, ASME winter annual meeting, December 1978Mechanical Design of Machine Elements and Machines, J.A. Collins, John Wiley & Sons, 2003 (Sec. 8.5)Example (7-3)By the end of Example 7-2, diameters 𝐷1 through 𝐷7 were determined. The layout is shown below(Figure 7-10). Here we are to evaluate the slopes and deflections at key locations.The text uses β€œBeam 2D Stress Analysis” (a software with FEA-core) for the evaluation.The results are verified by the above numerical integration method implemented with MATLAB.

DiameterExample 7-2𝐷1 𝐷71.0Point of InterestSlope, left bearing (A)Slope, right bearing (B)Slope , left gear (G)Slope, right gear (J)Deflection, left gear (G)Deflection, right gear (J)𝐷2 𝐷61.4Example 7-30.000501 rad0.001095 rad0.000414 rad0.000426 rad0.0009155 in0.0017567 in𝐷3 𝐷51.625𝐷42.0Numerical Integration0.000507 rad0.001090 rad0.000416 rad0.000423 rad0.0009201 in0.0017691 inHow to Determine Torsional (Angular) Deflection Important for shafts carrying components that are required to function in sync with each other; forexample, cam shafts; For a stepped shaft with individual cylinder length 𝑙𝑖 , torque 𝑇𝑖 and material 𝐺𝑖 the angulardeflection is,7-6 Critical Speeds for ShaftsIt is about applying knowledge of vibrations and deflections of shafts in the design of shafts.

The organization of this section:(Eq. 7-22): Exact solution of critical speed for a simply supported shaft with uniform cross section andmaterial(eq. 7-23): Rayleigh’s method to estimate critical speed.(Eq. 7-24): Through (Eq. 7-32) Derivation of Dunkerley’s method to estimate critical speed.(see pp. 376-377)

Example (7-5)Notes: (a) Rayleigh’s and Dunkerley’s methods only give rise to estimates; (b) They yield the upper andlower bound solutions, respectively. That is, πœ”1(π·π‘’π‘›π‘˜π‘’π‘Ÿπ‘™π‘’π‘¦) πœ”1 πœ”1(π‘…π‘Žπ‘¦π‘™π‘’π‘–π‘”β„Ž) ; (c) The methods andtheir derivations fall under vibrations/dynamics of continuum by energy method.Critical Speeds Critical speeds refer to speeds at which the shaft becomes unstable, such that deflections (due tobending or torsion) increase without bound. A critical speed corresponds to the fundamental natural frequency of the shaft in a particularvibration mode. Three shaft vibration modes are to be concerned: lateral, vibration, shaft whirling and torsionalvibration. Critical speeds for lateral vibration and shaft whirling are identical. Numerically speaking, two critical speeds can be determined, one for lateral vibration or shaftwhirling, and another for torsional vibration. Focus will be the critical speed for lateral vibration or shaft whirling. Regarding critical speed fortorsional vibration, one can reference β€œrotor dynamics” and the transfer matrix method. If the critical speed is πœ”1 , it is required that the operating speed πœ” be:If the shaft is rigid (shafts in heavy machinery):πœ” 3πœ”1If the shaft is flexible (shafts that are long with small-diameters):πœ” 1/3πœ”1The text recommends:πœ” 1/2πœ”1Exact solution, (Eq. 7-22)Simply supported, uniform cross-section and material.

Rayleigh’s Method for Critical Speed, (Eq. 7-23)Shaft is considered massless and flexible; Components such as gears, pulleys, flywheels, and so on, aretreated as lumped masses; The weight of the shaft, if significant, will be lumped as a mass or masses.Textbook equation should be updated to include the following absolute symbols:πœ”1 𝑔 𝑀𝑖 𝑦𝑖 𝑀𝑖 𝑦𝑖2Where:𝑀𝑖 weight of mass 𝑖𝑀𝑖 should be treated as a force with a magnitude equation the weight of mass 𝑖;Forces 𝑀𝑖 (𝑖 1, ) should be applied in such a way that the deflection curve resembles thefundamental mode shape of lateral vibration.𝑦𝑖 lateral deflection at location 𝑖 (where 𝑀𝑖 is applied) and caused by all forces.Dunkerley’s Method for Critical Speed, (Eq. 7-32)The model for Dunkerley’s method is the same as that for Rayleigh’s.𝑔and πœ”π‘–π‘– 𝑦𝑖𝑖 Where 𝑦𝑖𝑖 is the lateral deflection at location 𝑖 and caused by 𝑀𝑖 only. πœ”π‘–π‘– represents the critical speedwith only 𝑀𝑖 on the shaft.

Deflections π’šπ’Š π’šπ’Šπ’‹ and πœΉπ’Šπ’‹π‘¦π‘–π‘— is the deflection at location 𝑖 and due to a load applied at location 𝑗. When the load at location 𝑗 is aunit load, then 𝑦𝑖𝑗 is denoted by 𝛿𝑖𝑗 . 𝛿𝑖𝑗 is also known as the influence coefficient.𝑦𝑖 is the deflection at location 𝑖 and caused by all applied loads. Therefore,𝑦𝑖 𝑦𝑖𝑗𝑗unit load, then Type equation here.unit load, then 𝑦𝑖𝑗 is denoted at 𝛿𝑖𝑗 . 𝛿𝑖𝑗Problem SolvingClosed-form solutions (Sec. 4-4 and Table A-9).Superposition (Section 4-5);Indexes 𝑖 and 𝑗each runs 1 through the number of masses/forces;𝑦𝑖𝑗 are signed numbers;Example:Evaluate the range of the shaft’s critical speed corresponding to its lateral vibration, in terms of 𝐸𝐼where 𝐸𝐼 π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘.𝑖 1,2𝑗 1,2

From previous example:Table A 9{Case 10𝑦12 𝑦𝐴𝐡 π‘₯ 0.45 ( 700)(0.225)(0.45)(0.92 0452 )(6 0.9)𝐸𝐼7.9738𝐸𝐼𝑦22 𝑦𝑑 ( 700)(0.225)2 (0.9 0.225) 13.289 3𝐸𝐼𝐸𝐼Table A 9{Case 5𝑦11 π‘¦π‘šπ‘Žπ‘₯ 𝑦𝐴𝐡 (900)(0.9)3(13.669) 48𝐸𝐼𝐸𝐼𝐹π‘₯(4π‘₯ 2 3𝑙 2 )48πΈπΌπ‘‘π‘Œπ΄π΅πΉ(4π‘₯ 2 𝑙 2 ) ; 𝑑π‘₯16𝐸𝐼(900)( 0.92 )45.563πœƒπ΄ 16𝐸𝐼𝐸𝐼10.252𝑦21 ( πœƒπ΄ )(0.225) 𝐸𝐼Or:10.252𝑦21 (πœƒπΆ )(0.225) πΈπΌπœƒπ΄π΅ 0 π‘₯ 𝑙221.643𝐸𝐼23.541 𝐸𝐼 𝑦1 𝑦11 𝑦12 𝑦2 𝑦21 𝑦22Rayleigh’s Method:𝑔( 𝑀𝑖 𝑦𝑖 ) πœ”1 2( 𝑀𝑖 𝑦𝑖 )21.64323.541) (700) ()𝐸𝐼𝐸𝐼 (9.81)21.643 223.541 2(900) () (700) ()𝐸𝐼𝐸𝐼 0.66011 𝐸𝐼(900) (Dunkerley’s Method:13.669𝑦11 𝐸𝐼13.289𝑦22 𝐸𝐼𝑔2πœ”11 0.71768 𝐸𝐼 𝑦11

2πœ”22 𝑔 0.73820 𝐸𝐼 𝑦22 1112.74802 2 2 πΈπΌπœ”1 πœ”11 πœ”22πΈπΌπœ”1 0.60324 𝐸𝐼2.7480Take 𝐸 200 πΊπ‘ƒπ‘Ž, 𝑑 25 π‘šπ‘š 𝐸𝐼 1261.6 (𝑁 π‘š 2 ) πœ”1(π·π‘’π‘›π‘˜π‘’π‘Ÿπ‘™π‘’π‘¦) (0.60324)(1261.6) 761.0 π‘Ÿπ‘Žπ‘‘/π‘ π‘‚π‘Ÿ 𝑛1(π·π‘’π‘›π‘˜π‘’π‘Ÿπ‘™π‘’π‘¦) 7267 π‘Ÿπ‘π‘šπ΄π‘™π‘ π‘œ πœ”1(π‘…π‘Žπ‘¦π‘™π‘’π‘–π‘”β„Ž) 832.8 π‘Ÿπ‘Žπ‘‘/π‘ π‘‚π‘Ÿ 𝑛1(π‘…π‘Žπ‘¦π‘™π‘’π‘–π‘”β„Ž) 7952 π‘Ÿπ‘π‘š π‘‚π‘π‘’π‘Ÿπ‘Žπ‘‘π‘–π‘›π‘” 𝑆𝑝𝑒𝑒𝑑 1πœ”3 1π‘‚π‘Ÿ 𝑛 2422 π‘Ÿπ‘π‘š7-3 Shaft Layout Between a shaft and its components (e.g., gears, bearings, pulleys, etc.), the latter must be locatedaxially and circumferentially. Means to provide for torque transmissionKeysSplinesSetscrewsPinsPress/shrink fitsTapered fitsetc. Means to provide for axial location – large axial load shouldersShouldersRetaining ringssleevesCollarsetc. Means to provide for axial location – small axial loadPress/shrink fitsSetscrewsetc. Locating rolling element bearingsSee Ch. 11

7-7 Miscellaneous Shaft ComponentsIncludes:- Setscrews- Keys and pins- Retaining ringsFocus:KeysExample 7-67-8 Limits and Fits Fits (clearance, transition, and interference) are to ensure that a shaft and itscomponents/attachments will function as intended. Preferred fits are listed in Table 7-9 Medium drive fit and force fit will give rise to the press/shrink fits. Press-fit is typically for small hubs; Shrink fit (or expansion fit) it used with larger hubs How much diameter interference to have?0.001” for up to 1” of diameter0.002” for diameter 1” to 4” Press/shrink fits can be designed to transfer torque and axial load. Press/shrink fits are known to be associated with fretting corrosion (loss of material from theinterface) (Section 3-14) for stress distributions in thick-walled cylinder under pressures. (Section 3-16) for stresses developed in the shaft and hub due to pressure induced by a press/shrinkfit; or (Eq 7-39) to (Eq. 7-47) Axial load and torque capacities: (Eq. 7-48) and (Eq. 7-49) Radial interference versus diametral interference (not necessarily the same thing).

Chapter 11: Rolling-Contact BearingsPart 1: (Introduction)11-1 Bearing TypesPart 2: (The Basics)11-2 Bearing Life11-3 Bearing Life at Rated Reliability11- 4Reliability versus Life – The Weibull Distribution11-5 Relating Bearing Load, Life and ReliabilityPart 3: (Selection of Bearing)11-6 Combined Radial and Thrust Bearing11-8 Selection of Ball and Roller Bearings11-7 Variable Loading11-10 Design AssessmentPart 4: Others11-12 Mounting and Enclosure11-11 Lubrication11-9 Selection of Tapered Roller Bearings11-1 Bearing TypesNomenclatureSee Figure 11-1Classifications By shape of rolling elements (sphere, cylinder, tapered, etc.) By type of loads taken (radial only, axial only, combination) By permissible slope (Self-aligning, non-self-aligning) Sealed? Shielded? Figures 11-2, 11-3

11-2 Bearing LifeWhy Bearing Life? Bearings are under cyclic contact stresses (compressive as well as shear). As a result, they mayexperience crack, putting, spalling, fretting, excessive noise, and vibration. Common life measures are:o Number of revolutions of the inner ring (outer ring stationary) until the first evidence offailure; ando Number of hours of use at standard angular speed until the first evidence of fatigue Number of revolutions is more common

Rating Life (or Rated Life) This is the terminology used by ABMA (American Bearing Manufacturers Association) and mostbearing manufacturers. It is defined as, of a group of nominally identical bearings, the number of revolutions that 90% of thebearings in the group will achieve or exceed, before failure occurs. It is denoted as 𝐿10 or 𝐡10 life. The typical value for 𝐿10 or 𝐡10 is 1 million. However, a manufacturer can choose its own specific rating life. For example, Timken uses 90 million for tapered roller bearings, but 1 million for its other bearings. Refer to bearings catalog for value(s) of 𝐿10 .11-3 Bearing Life at Rated Reliability At rated reliability of 90%, bearing life 𝐿 relates to bearing’s radial load 𝐹 by:𝐹𝐿1/π‘Ž π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘Where π‘Ž 3 for ball bearings and π‘Ž 10/3 or roller bearings.Figure 11-4 shows the meaning of (Eq. 11-1) o It’s a straight line on log-log scales;o Points on the line will have the same reliability;o The line corresponding to 90% reliability is called the rated line.To determine the constant on the RHS of (Eq. 11-1), 𝐿 is set to 𝐿10 . The corresponding 𝐹 isdesignated as 𝐢10 .𝐢10 is called the Basic Dynamic Load Rating, or the Basic Dynamic Rated Load It is defined as theradial load that causes 10% of the group of nominally identical bearings to fail at or before 𝐿10(1 million, or 90 million, or revs as chosen by a manufacturer).(Equation 11-1) becomes:1/π‘Ž1/π‘ŽπΉπ· 𝐿𝐷 𝐢10 𝐿10(11 3)

Where the subscript 𝐷 means design. (Equation 11-3)* is essentially (Eq. 11-3) of the text. In (Eq. 11-3),the subscript 𝑅 means rated. Example 11-1: find 𝐢10 from known 𝐿𝐷 , 𝐹𝐷 and 𝐿1011-4 Reliability versus Life – The Weibull Distribution11-5 Relating Load, Life and Reliability At 90% reliability, (Eq. 11-3*) forms the basis for selecting a bearing. What if the reliability is not 90%?Figure 11-5 shows the process of going from the rated line to a different line.𝐴 𝐷, with 𝐡 being the intermediary. 𝐴 𝐡: Load is constant, and life measure (which is a random variable) follows a three-parameterWeibull distribution𝐡 𝐷: Reliability is constant, and (Eq. 11-3*) is valid; The mathematics is given in (Sec. 11-4) and(Sec. 11-5).Another approach is to use a reliability factor π‘Ž1 , the value of which depends on 𝑅, the reliability.Values of π‘Ž1 are available from a number of references.R, %909596979899 Reliability Factor, π’‚πŸ1.000.620.530.440.330.21The factor π‘Ž1 can be determined by (courtesy of, for example SKF catalog)100 2/3π‘Ž1 4.48 (ln)𝑅Where 𝑅 is in %, e.g., 𝑅 92.5. Note: 𝑅 99.

Timken recommends the following formula for π‘Ž1100 2/3π‘Ž1 4.26 (ln) 0.05𝑅Where 𝑅 99.9The Basic Bearing EquationThe basic bearing equation can now be obtained by, in (Eq. 11-3), introducing the reliability factor π‘Ž1and a load-application factor π‘˜π‘Ž . That is,1/π‘Ž1/π‘ŽπΉπ· 𝐿𝐷 𝐢10 𝐿10Becomes,𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10π‘˜π‘Ž is given in (Table 11-5)This basic equation can be used for bearing selection and for assessment after selection.Example 1A SKF deep-groove ball bearing is subjected to a radial load of 495 lb. The shaft rotates at 300 rpm. Thebearing is expected to last 30,000 hours (continuous operation). Catalog shows a 𝐢10 19.5 π‘˜π‘ on thebasis of 106 revs. (1) is the bearing suitable for 90% reliability? (2) Also assess the bearing’s reliability.Set π‘˜π‘Ž 1.Solution:The basic bearing equation is:𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10(Where π‘Ž and 𝐿10 are generally set by the manufacturer, π‘˜ is a variable we can change.)Where:𝐢10 19.5 π‘˜π‘ 4387.5 𝑙𝑏; 𝐿10 106 π‘Ÿπ‘’π‘£π‘ ; π‘˜π‘Ž 1; π‘Ž 3Also 𝐹𝐷 495 𝑙𝑏; and 𝐿𝐷 (30,000)(60)(300) (540)(106 ) π‘Ÿπ‘’π‘£π‘ .Assume 90% reliability, then π‘Ž1 1. From the basic bearing equation,𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10Substituting values, 𝐿𝐻𝑆 8.92, 𝑅𝐻𝑆 8.14. Therefore, (𝐿𝐷 , 𝐹𝐷 ) is not on the rated line.

There are a number of ways to seek the answer.90% reliability, π‘Ž1 1;The first: similar to the typical calculations done for selecting a bearingSet 𝐹𝐷 495 𝑙𝑏; 𝐿𝐷 (540)(106 ) π‘Ÿπ‘’π‘£π‘ ; and 𝐿10 106 π‘Ÿπ‘’π‘£π‘ ; find 𝐢10 and check if it is less than the4387.5 𝑙𝑏 that the bearing is capable of providing.From:𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10Substituting known values:1/3𝐢10(540)(106 ) ()(1)(106 )(1)(495)Resulting in 𝐢10 4031 𝑙𝑏Since it’s less than the catalog’s 𝐢10 , or 4387.5 𝑙𝑏, the selected bearing is suitable for 90% reliability.The second: can be used to select a bearing (pre-selecting a bearing, then checking to make sure it issuitable)Set 𝐿𝐷 (540)(106 ) π‘Ÿπ‘’π‘£π‘ , find 𝐹𝐷 , and check is 𝐹𝐷 495 𝑙𝑏.From:𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10Substituting known values:1/3(4387.5)(540)(106 ) ()(1)(106 )(1)𝐹𝐷Solving gives 𝐹𝐷 538.8 𝑙𝑏 with 90% reliability and a life of (540)(106 ) π‘Ÿπ‘’π‘£π‘ , the bearing can take on a maximum radial load of538.8 𝑙𝑏. Since the applied radial load is only 495 𝑙𝑏, the bearing will have better than 90% reliability.The third: similar to post-selection calculation to evaluate the life of the bearing.Set 𝐹𝐷 495 𝑙𝑏, find 𝐿𝐷 , and check if 𝐿𝐷 (540)(106 ) π‘Ÿπ‘’π‘£π‘ .From:𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10Substituting known values:1/3(4387.5)𝐿𝐷 ()(1)(106 )(1)(495)Solving gives 𝐿𝐷 (696)(106 ) π‘Ÿπ‘’π‘£π‘ With a radial load at 495 𝑙𝑏, the bearing has 90% chance proabability to survive at least(696)(106 ) π‘Ÿπ‘’π‘£π‘ . The chance of surviving only (540)(106 ) π‘Ÿπ‘’π‘£π‘  is better than 90%.(2) Set 𝐹𝐷 495 𝑙𝑏; 𝐿𝐷 (540)(106 ) π‘Ÿπ‘’π‘£π‘ To assess reliability means to evaluate π‘Ž1 . This is typically done after selection.

From:𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10Substituting known values:1/3(4387.5)(540)(106 ) ()(1)(495)π‘Ž1 (106 )Solving gives π‘Ž1 0.775Finally, from:π‘Ž1 4.26 (ln100 2/3) 0.05𝑅Solving for 𝑅 results in 𝑅 93%.With the radial load at 495 𝑙𝑏, there is a 7% of chance that the bearing would fail at or before 540millions of revs.It shows that the bearing is more than suitable for 90% reliability.Example 2Select bearings A and B for the shaft of Example 7-2. They are to be used for a minimum of 1,000 hoursof continuous operation. Shaft rpm is 450. Radial loads are, 𝐹𝐴 375 𝑙𝑏 and 𝐹𝐡 1918 𝑙𝑏. Shaftdiameter at both locations is 1" (𝐷1 and 𝐷7 in Figure 7-10). Assume 90% reliability.Solution:Table 11-2Table 11-3Since there is no thrust load, deep-groove ball bearings may

Example 2Select bearings A and B for the shaft of Example 7-2. They are to be used for a minimum of 1,000 hoursof continuous operation. Shaft rpm is 450. Radial loads are, 𝐹𝐴 375 𝑙𝑏 and 𝐹𝐡 1918 𝑙𝑏. Shaftdiameter at both locations is 1" (𝐷1 and 𝐷7 in Figure 7-10). Assume 90% reliability.Solution:Since there is no thrust load, deep-groove ball bearings are first considered. Table 11-2 has a list of 02series deep groove ball bearings.π‘Ž1 1;π‘˜π‘Ž 1.2 (π‘‡π‘Žπ‘π‘™π‘’ 11 5, π‘π‘œπ‘šπ‘šπ‘’π‘Ÿπ‘π‘–π‘Žπ‘™ π‘”π‘’π‘Žπ‘Ÿπ‘–π‘›π‘”, 1.1 1.3);𝐿10 106 π‘Ÿπ‘’π‘£π‘ ;𝐿𝐷 1000 60 450 27 106 π‘Ÿπ‘’π‘£π‘ ;

Bearing 𝐡: 𝐹𝐷 𝐹𝐡 1918 𝑙𝑏 8535 𝑁. From:𝐢10𝐿𝐷 1/π‘Ž ()π‘˜π‘Ž πΉπ·π‘Ž1 𝐿10It’s found that 𝐢10 30,726 𝑁. Note π‘Ž 3.Table 11-2 Shows that the smallest (in dimensions) bearing meeting the requirements is the one withbore diameter of 40 π‘šπ‘š and its 𝐢10 is 30.7 π‘˜π‘.Switch to roller bearing (Table 11-3). With π‘Ž 10/3, then 𝐢10 27,529 𝑁.From Table 11-3, under 02-series, the bearing with 35-mm bore has 𝐢10 31.9 𝑁;Under 03 series, the bearing with 25-mm bore has a 𝐢10 28.6 kN.

Select 03-series, π‘π‘œπ‘Ÿπ‘’ 25 π‘šπ‘š, 𝑂𝐷 62 π‘šπ‘š, π‘€π‘–π‘‘π‘‘β„Ž 17 π‘šπ‘š, and 𝐢10 28.6 π‘˜π‘Assessing reliability: π‘Ž1 0.88, and 𝑅 91.7Bearing 𝐴: 𝐹𝐷 𝐹𝐴 375 𝑙𝑏 1669 𝑁. Use the same bearings as at B.Assessing reliability: π‘Ž1 0.00382, 𝑅 99.9975. So 𝑅 99.The two bearings combined will have a reliability of (0.917) (0.99) 0.9111-6 Combine

Chapter 6: Fatigue Failure (Review) I) Sec 6-17 Road Maps and Important Equations II) Loading Simple loading - Axial loading - Torsion - Bending Combined Loading III) Characterizi

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