Endurance Strength Pg 274

Similar documents
DESIGN FOR FATIGUE STRENGTH

Failure from static loading

Fatigue Life. The curve may be plotted as semilogarithmic

MEMS Project 2 Assignment. Design of a Shaft to Transmit Torque Between Two Pulleys

FME461 Engineering Design II

Static Failure (pg 206)

Shafts. Fig.(4.1) Dr. Salah Gasim Ahmed YIC 1

Path to static failure of machine components

Stress Analysis Lecture 3 ME 276 Spring Dr./ Ahmed Mohamed Nagib Elmekawy

Design against fluctuating load

Mechanical Design. Design of Shaft

Chapter 10 1" 2 4" 1 = MPa mm. 201 = kpsi (0.105) S sy = 0.45(278.7) = kpsi D = = in. C = D d = = 10.

CHAPTER 2 Failure/Fracture Criterion

Chapter 8 Structural Design and Analysis. Strength and stiffness 5 types of load: Tension Compression Shear Bending Torsion

Springs Lecture 3. Extension Springs

DESIGN OF SHAFT UNDER FATIGUE LOADING

MAE 322 Machine Design. Dr. Hodge Jenkins Mercer University

Sample Questions for the ME328 Machine Design Final Examination Closed notes, closed book, no calculator.

Experiment: Torsion Test Expected Duration: 1.25 Hours

2.1 Background of Piping Stresses

Load Determination. Fatigue Life Predictions Infinite Life, Stress Life, Strain Life

Solid Mechanics Homework Answers

ME 2570 MECHANICS OF MATERIALS

BME 207 Introduction to Biomechanics Spring Homework 9

Design and analysis of axle under fatigue life loading condition

[5] Stress and Strain

PROBLEM 7.1 SOLUTION. σ = 5.49 ksi. τ = ksi

Variable Stresses in Machine Parts

Fatigue Problems Solution

FCP Short Course. Ductile and Brittle Fracture. Stephen D. Downing. Mechanical Science and Engineering

Note: Read section (12-1) objective of this chapter (Page 532)

Volume 2 Fatigue Theory Reference Manual

Fatigue Algorithm Input

This guide is made for non-experienced FEA users. It provides basic knowledge needed to start your fatigue calculations quickly.

ME 243. Mechanics of Solids

Local Buckling. Local Buckling in Columns. Buckling is not to be viewed only as failure of the entire member

Examination of the Fatigue Life under Combined Loading of Specimens

Sean Carey Tafe No Lab Report: Hounsfield Tension Test

Introduction to Engineering Materials ENGR2000. Dr. Coates

Constitutive Equations (Linear Elasticity)

Determine the resultant internal loadings acting on the cross section at C of the beam shown in Fig. 1 4a.

1.3 Working temperature T 200,0 1.4 Working environment. F... Guided seating. Light service. Cold formed springs. Music wire ASTM A228

CHAPTER 8 SCREWS, FASTENERS, NONPERMANENT JOINTS

Module 5: Theories of Failure

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola

Fatigue calculations in ANSYS Workbench. Martin Eerme

The mean stress influence on lifetime under high-cycle fatigue combined loading

MMJ1133 FATIGUE AND FRACTURE MECHANICS A - INTRODUCTION INTRODUCTION

Examination in Damage Mechanics and Life Analysis (TMHL61) LiTH Part 1

Chapter 1 Introduction- Concept of Stress

NORMAL STRESS. The simplest form of stress is normal stress/direct stress, which is the stress perpendicular to the surface on which it acts.

4. SHAFTS. A shaft is an element used to transmit power and torque, and it can support

ME 354 MECHANICS OF MATERIALS LABORATORY STRESSES IN STRAIGHT AND CURVED BEAMS

The science of elasticity

Aluminum shell. Brass core. 40 in

Stress concentrations, fracture and fatigue

MECHANICS OF MATERIALS

SOLUTION (17.3) Known: A simply supported steel shaft is connected to an electric motor with a flexible coupling.

MECHANICS OF MATERIALS

12/25/ :27 PM. Chapter 14. Spur and Helical Gears. Mohammad Suliman Abuhaiba, Ph.D., PE

Members Subjected to Combined Loads

A fatigue limit diagram for plastic rail clips

MECE 3321 MECHANICS OF SOLIDS CHAPTER 3

Outline. Tensile-Test Specimen and Machine. Stress-Strain Curve. Review of Mechanical Properties. Mechanical Behaviour

Stress Analysis of a Compressor Vane-Spring

The University of Melbourne Engineering Mechanics

ME311 Machine Design

Chapter 7. Highlights:

Mechanics of Materials

Engineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS

INTRODUCTION (Cont..)

Drive Shaft Failure of Z-Drive Propulsion System. Suzanne Higgins

MAE 322 Machine Design Lecture 2. Dr. Hodge Jenkins Mercer University

Samantha Ramirez, MSE. Stress. The intensity of the internal force acting on a specific plane (area) passing through a point. F 2

Fundamentals of Durability. Unrestricted Siemens AG 2013 All rights reserved. Siemens PLM Software

My conrod model can be found on the CD enclosed with this assignment.

Software Verification

MECHANICS OF MATERIALS

DESIGN & STATIC STRUCTURAL ANALYSIS OF CRANKSHAFT FOR HIGH PRESSURE PLUNGER PUMP

Problem d d d B C E D. 0.8d. Additional lecturebook examples 29 ME 323

5. STRESS CONCENTRATIONS. and strains in shafts apply only to solid and hollow circular shafts while they are in the

Design and Finite Element Analysis of Crank Shaft by using Catia and Anysys

Torsion of Shafts Learning objectives

Downloaded from Downloaded from / 1

Mechanics of Materials CIVL 3322 / MECH 3322

Tuesday, February 11, Chapter 3. Load and Stress Analysis. Dr. Mohammad Suliman Abuhaiba, PE

DESIGN OF BEAMS AND SHAFTS

High Cycle Fatigue Estimation of Aircraft Exhaust T50 Thermocouple Siddesha T 1 Dr. B Ravindra 2

INFLUENCE OF HYDROSTATIC PRESSURE ON MULTIAXIAL FATIGUE OF NOTCHED COMPONENTS. G. Qilafku, G. Pluvinage

6.37 Determine the modulus of resilience for each of the following alloys:

Fatigue and Fracture

five Mechanics of Materials 1 ARCHITECTURAL STRUCTURES: FORM, BEHAVIOR, AND DESIGN DR. ANNE NICHOLS SUMMER 2017 lecture

Multiaxial Fatigue. Professor Darrell F. Socie. Department of Mechanical Science and Engineering University of Illinois at Urbana-Champaign

2. Rigid bar ABC supports a weight of W = 50 kn. Bar ABC is pinned at A and supported at B by rod (1). What is the axial force in rod (1)?

Design Parameter Sensitivity Analysis of High-Speed Motorized Spindle Systems Considering High-Speed Effects

12/8/2009. Prof. A.K.M.B. Rashid Department of MME BUET, Dhaka

ME111 Instructor: Peter Pinsky Class #21 November 13, 2000

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA MECHANICAL PRINCIPLES AND APPLICATIONS NQF LEVEL 3 OUTCOME 1 - LOADING SYSTEMS TUTORIAL 3 LOADED COMPONENTS

MATERIALS FOR CIVIL AND CONSTRUCTION ENGINEERS

Transcription:

[Pg / 8] Fatigue Analysis Pg 257 The Units used as standard: in, kip, kpsi, sec, hp in, kip, kpsi, sec/min, hp Endurance Strength Pg 274 Fatigue failure occurs when a machine element is sujected to fluctuating load. The inherent strength of the material weaken at every cycle until eventually the structure is overcome y the applied cyclic load. To determine the strength of material under fatigue loading, specimens are sujected to repeated loading of specified magnitude and counted to destruction. The most widely used is the R. R. Moore machine fatigue test. Aove: Moores' Fatigue Test machine Below: SN diagrams from Moores' experiment

[Pg 2 / 8] # S-N DIAGRAM: Endurance (fatigue) strength against numer of cycles of Moore's steel specimen. See Fig 6-0 Pg 266 # Below: SN graph of other metals under fatigue load.

[Pg 3 / 8] Endurance Strength @ Infinite Life Endurance Limit ' = 0.5S ut if S ut 400MPa (See Eqn 6-8 pg 274) NB: Endurance limits found only in steel and titanium Endurance Limit Modifying Factors Pg 278 Surface factor, k a as ut = 0.265 Eg: If surface is machined: k a = 4.5S ut Size factor for round and rotating shaft, k =.24d 0.07 if 2.79 d 5mm k =.5d 0.57 if 5 < d 254mm Load factor, k c = ==> ending load k c = 0.85 (for ending and axial load comined) Temperature factor, k d, Reliaility factor, k e, Misc factor, k f = Endurance Limits, = k a k k c k d k e k f '

[Pg 4 / 8] CYCLIC LOADINGS Pg 292 Static Load is applied slowly without shock and is held at constant value. Repeated and Reversed Reversed: when a load-carrying component is sujected to certain level of tensile load followed y a same level of compressive load. Repeated: when loading is repeated many thousand times. σ max - maximum stress acting on the specimen σ min - minimum stress acting on the specimen τ max - maximum shear stress acting on the specimen τ min - minimum shear stress acting on the specimen K f - stress concentration factor mean stress acting on the specimen σ max + σ min σ m = K f 2 alternating stress acting on the specimen σ max σ min σ a = K f 2

[Pg 5 / 8] STRESS CONCENTRATION Pg 287 K t theoritical stress concentration factor Pg 05 See Tale A-5 to A-6 K f q = notch sensitivities. (concentration factor are less severe for some materials). K t See Fig 6-20, 6-2 and eqn. 6-32 & 6-33. For Cast Iron: q = 0.2 ( ) K f = + q K t actual stress concentration factor (reduced value of Kt due to different material type ie different notch sensitivities) σ t = K f σ n SC stress (at Stress Concentration region) Sample Prolem Given : P = 5kN Cross section area : A n = ( 25mm) ( 25mm) = 625 mm 2 P Normal stress (without notch), σ n = = 24 0 6 Pa Stress concentration occurs at notch : See pg 003 Fig A-3-3 : A n r d 2.5mm = = 0. 25mm w d 30mm = =.2 K t = 2.38 25mm S ut = 400MPa r f = 2mm q = 0.73 ( ) K f = + q K t = 2.007 Cross section area at notch region : A t = ( 25mm) ( 25mm 5mm) = 500 mm 2 P Actual stress at notch : σ t = K f = 60.27 MPa A t

[Pg 6 / 8] Fatigue Failure Criterion Pg 297 Langer's eqn (for early cycle yielding) : σ a S y + σ m S y = [6-48] η Modified Goodman equation: σ a + σ m S ut = [6-45] η Gerer equation: ησ a 2 ησ m + = [6-46] S ut Sodererg equation: σ a + σ m S y = [6-44] η If η =.0 then the stress (σ m,σ a ) lies on the Langer line or the other fatigue curves. Any points lower than the curves are safe i.e. η >.0. To ensure the materials do not yield at the first cycle loading, the Langer's equation must e applied against oth stresses σ m, σ a. If the material is considered safe y Langer, further analysis must done using any of the Fatigue equations as can e explained y the figure elow. The Sodererg lines is an exception to the aove ecause it does need to e accompanied y Langer's test.

[Pg 7 / 8] Fatigue Strength @ Finite Life Pg 276 Method : To find the finite life, we need the equation S f = an x Total numer. of cycles, N x < 000000 If S ut < 490MPa then f = 0.9 If 490 S ut 400MPa get f from Fig 6-8 pg 277 ( ) 2 fs ut a = = log fs ut 3 σ a if σ m = 0 then N x = a If σ m 0 then do the following steps: Apply modified Goodman equation: Use the equation derived from S f σ a S f σ m + = to get S f S ut S f = an x that is, N x = a

[Pg 8 / 8] Stress Concentration Factor at Finite Life K 3 = K f ( ) Sut ( ) 0.8 0.43 0 2 ( ) Sut 2 + 0.45 0 5 2 K 3 3 log K N = N x K f K f K 3 From the figure aove, when the mean stress is compressive, failure occurs when σ a = In a complete setup, the figure elow shows the safe area for Goodman Fatigue life.