Materials Issues in Fatigue and Fracture. 5.1 Fundamental Concepts 5.2 Ensuring Infinite Life 5.3 Failure 5.4 Summary

Similar documents
III Fatigue Models. 1. Will a crack nucleate? 2. Will it grow? 3. How fast will it grow?

STRENGTHENING MECHANISM IN METALS

Chapter Outline Dislocations and Strengthening Mechanisms. Introduction

Chapter Outline: Failure

Design of High Strength Wrought Magnesium Alloys!

Mechanical Properties

1) Fracture, ductile and brittle fracture 2) Fracture mechanics

Quiz 1 - Mechanical Properties and Testing Chapters 6 and 8 Callister

Fatigue of metals. Subjects of interest

Module-6. Dislocations and Strengthening Mechanisms

Introduction to Engineering Materials ENGR2000 Chapter 8: Failure. Dr. Coates

Tensile Testing. Objectives

21 Fracture and Fatigue Revision

APPLIED ENGINEERING PRINCIPLES MANUAL

Engineering 45: Properties of Materials Final Exam May 9, 2012 Name: Student ID number:

A DISLOCATION MODEL FOR THE PLASTIC DEFORMATION OF FCC METALS AN ANALYSIS OF PURE COPPER AND AUSTENITIC STEEL

Hall-Petch Analysis from a Combined Mechanics and Materials Viewpoint

Heat Treatment of Steel Lab Report. Justin Lance 11/16/2011 Engineering 45 Lab Section 3 Troy Topping

Technologies for Process Design of Titanium Alloy Forging for Aircraft Parts

Mechanical behavior of crystalline materials - Stress Types and Tensile Behaviour

Analysis of low cycle fatigue in AlMgSi aluminium alloys

Uniaxial Ratcheting Behaviors of Metals with Different Crystal Structures or Values of Fault Energy: Macroscopic Experiments

Lectures on: Introduction to and fundamentals of discrete dislocations and dislocation dynamics. Theoretical concepts and computational methods

Precipitation Hardening. Outline. Precipitation Hardening. Precipitation Hardening

Mechanical Properties of Metals. Goals of this unit

Progress Since the Last TIM (July 98) (On Modeling Corrosion Damage)

arxiv: v1 [cond-mat.mtrl-sci] 8 Nov 2016

Cyclic Fatigue Testing of Wrought Magnesium AZ80 Alloy for Automotive Wheels

MATERIALS SCIENCE-44 Which point on the stress-strain curve shown gives the ultimate stress?

a. 50% fine pearlite, 12.5% bainite, 37.5% martensite. 590 C for 5 seconds, 350 C for 50 seconds, cool to room temperature.

Defects and Diffusion

A THERMOMECHANICAL FATIGUE CRACK INITIATION MODEL FOR DIRECTIONALLY-SOLIDIFIED NI-BASE SUPERALLOYS

Prediction of fatigue crack propagation in aluminum alloy with local yield strength gradient at the crack path

MICROSTRUCTURAL INVESTIGATION OF SPD PROCESSED MATERIALS CASE STUDY

Problem Set 2 Solutions

Creep and High Temperature Failure. Creep and High Temperature Failure. Creep Curve. Outline

Recrystallization Theoretical & Practical Aspects

Thin Products < 75 mm 7055-T7751. Strength (MPa) 500. Thick Products mm Year First Used in Aircraft

Plastic Deformation in Crystalline Materials. Lecture 1: Overview. Kamyar Davoudi Fall 2015

Phase Transformations in Metals Tuesday, December 24, 2013 Dr. Mohammad Suliman Abuhaiba, PE 1

A study of dislocation evolution in polycrystalline copper during low cycle fatigue at low strain amplitudes

Learning Objectives. Chapter Outline. Solidification of Metals. Solidification of Metals

Designing martensitic steels: structure & properties Enrique Galindo-Nava and Pedro Rivera

Chapter 2 General Mechanisms of Creep

Dislocations and Plastic Deformation

EFFECT OF THE LCF LOADING CYCLE CHARACTERISTICS ON THE FATIGUE LIFE OF INCONEL 718 AT HIGH TEMPERATURE

Materials Engineering 272-C Fall 2001, Lectures 9 & 10. Introduction to Mechanical Properties of Metals

Objective To study the time and temperature variations in the hardness of Al-4% Cu alloy on isothermal aging.

DOE FUNDAMENTALS HANDBOOK

Modern Creep Lifing Techniques for Gas Turbine Research

Modeling and simulation of temperature-dependent cyclic plastic deformation of austenitic stainless steels at the VHCF limit

The Microstructure and Mechanical Properties of Inconel 718 Fine Grain Ring Forging

Available online at ScienceDirect. Procedia Engineering 160 (2016 ) 85 92

Planar Defects in Materials. Planar Defects in Materials

PowerPoint Images. Chapter 7. Failures Resulting from Variable Loading. Shigley Mischke Budynas. Mechanical Engineering Design Seventh Edition

THE EFFECT OF TEMPERATURE AND MEAN STRESS ON THE FATIGUE BEHAVIOUR OF TYPE 304L STAINLESS STEEL INTRODUCTION

Energy and Packing. Materials and Packing

AN OVERVIEW OF THE HISTORY OF PLASTICITY THEORY

ME -215 ENGINEERING MATERIALS AND PROCESES

The University of Jordan School of Engineering Chemical Engineering Department

Free Electron Model What kind of interactions hold metal atoms together? How does this explain high electrical and thermal conductivity?

Mechanical Behavior of Plutonium and Its Alloys

INFLUENCE OF SECUNDARY AGEING ON MECHANICAL PROPERTIES OF AN AA7050 ALUMINUM ALLOY

Imperfections: Good or Bad? Structural imperfections (defects) Compositional imperfections (impurities)

Microstructural parameters from Multiple Whole Profile (MWP) or Convolutional Multiple Whole Profile (CMWP) computer programs

MICROMECHANISMS OF CLEAVAGE FRACTURE IN THE HAZ OF C-MN COMMERCIAL STEEL WELD

MAE 322 Machine Design Lecture 5 Fatigue. Dr. Hodge Jenkins Mercer University

Deformation Twinning in Bulk Aluminum with Coarse Grains

Materials Science Handbook: Volume 1 Structure and Properties of Metals 5 PDH / 5 CE Hours

Free Electron Model What kind of interactions hold metal atoms together? How does this explain high electrical and thermal conductivity?

Materials! Solidification Processes!

sample initial height

Fundamentals of Material Science

Laboratory 3 Impact Testing of Metals

Formability and Crystallographic Texture in Novel Magnesium Alloys

Practice Problems Set # 3 MECH 321 Winter 2018

The heat treatment of austenitic stainless steel wire with different work hardening degree

The strength of a material depends on its ability to sustain a load without undue deformation or failure.

Effect of Ti on Charpy Fracture Energy and Other Mechanical Properties of ASTM A 710 Grade B Cu-Precipitation-Strengthened Steel

Impurities in Solids. Crystal Electro- Element R% Structure negativity Valence

Mechanical behavior of crystalline materials- Comprehensive Behaviour

Module #25. Martensitic Transformations and Strengthening

FATIGUE PROPERTIES OF NICKEL-BASE SUPERALLOY INCONEL 792-5A AT 800 C

Index. Atmosphere Effect on fatigue processes, 49, 200 Auger spectroscopy, 51 A533-B steel Mode II fracture, 235, 242 B

Fatigue life estimation of Aluminium Alloy reinforced with SiC particulates in annealed conditions

Chapter 8 Deformation and Strengthening Mechanisms. Question: Which of the following is the slip system for the simple cubic crystal structure?

Fatigue crack initiation in Hastelloy X the role of boundaries

Single-Crystal Plasticity

Cold Spray Developments at UTRC

Chapter 11. Mechanical Behavior of Materials

Institutional repository of Jönköping University

Chapter Outline How do atoms arrange themselves to form solids?

Experiment E: Martensitic Transformations

Behaviour of Magnesium Alloy Under Load-Control Cyclic Testing

PLASTIC DEFORMATION AND THE ONSET OF TENSILE INSTABILITY

CHAPTER 6: MECHANICAL PROPERTIES ISSUES TO ADDRESS...

THEORY QUESTIONS [60% of paper for weld fatigue]

History and Future of High-Fatigue-Strength Steel Wire for Automotive Engine Valve Spring

CHAPTER 3 OUTLINE PROPERTIES OF MATERIALS PART 1

Characteristics affecting each stage of fatigue fracture

Transcription:

Materials Issues in Fatigue and Fracture 5.1 Fundamental Concepts 5.2 Ensuring Infinite Life 5.3 Failure 5.4 Summary 1

A simple view of fatigue 1. Will a crack nucleate? 2. Will it grow? 3. How fast will it grow? Cyclic nucleation and arrested growth Crack growth 2

5.2 Ensuring Infinite Life Avoiding crack nucleation Avoiding crack growth Fatigue limit and the UTS UTS of structural materials 3

Avoiding crack nucleation Smooth specimen Infinite life At a sufficiently low alternating stress no fatigue cracks will form. 4

Cyclic hardening Development of cell structures (hardening) Increase in stress amplitude (under strain control) Break down of cell structure to form PSBs Localization of slip in PSBs cyclic hardening cyclic softening PSB 5

Cyclic Deformation Hysteresis loops? ε 6

Cyclic stress-strain curve? ε σ Cyclic stressstrain curve ε = σ E + σ K' 1/n' ε ε = σ E +2 σ 2K' 1/n' Hysteresis loops for different levels of applied strain 7

Cyclic stress-strain curves Maximum stress amplitude for infinite life. ε = σ E + σ K' 1/n' ε = σ E + σ K 1/n 8

5.2 Ensuring Infinite Life Avoiding crack nucleation Avoiding crack growth Fatigue limit and the UTS UTS of structural materials 9

Infinite life - no crack growth Infinite life Sharp notches may nucleate cracks but the remote, alternating stress may not be large enough to cause the crack to leave the notch stress field. 10

Threshold Stress Intensity The forces driving a crack forward are related to the stress intensity factor a?s At or below the threshold value of?k, the crack doesn t grow. K = Y S πa 11

Non-propagating cracks Endurance limit for smooth specimens Stress range,?s Non-propagating cracks Failure a th = 1 π K th S 2 Crack length 12

5.2 Ensuring Infinite Life Avoiding crack nucleation Avoiding crack growth Fatigue limit and the UTS UTS of structural materials 13

Fatigue limit related to UTS For wrought steel the fatigue strength at 1,000,000 cycles is about 0.5 UTS. For wrought aluminum the fatigue strength at 10,000,000 cycles is about 0.35 UTS. 14

5.2 Ensuring Infinite Life Avoiding crack nucleation Avoiding crack growth Fatigue limit and the UTS UTS of structural materials 15

Theo. shear stress of a solid τ τ + + + + ao + + + x + b 2b τ b τm G 2š slip plane For iron (Fe), the theoretical shear stress is about 2,000,000 psi!?! 16

Dislocations τ y = G e 2πw b G e 4π 50 psi.!!! (Pierels stress) The concept of the dislocation explains why the theoretical shear strength is never achieved. However, dislocation theory would predict very low flow stresses!?! Pierels stress. 17

Strengthening mechanisms τ y = τ Pieierls + τ solution + τ dispersion + τ hardening Flow stress of a single crystal τ y solution α C 1 / 2 Solid solution strengthening - atomic misfits set up dislocation impeding stress fields 18

Strengthening mechanisms τ y dispersion = 2 T b L = G b L Dispersion (precipitate) strengthening - small second phase particles impede dislocation motion. 19

Strengthening mechanisms τ y hardening α γ m Work hardening - increasing number of dislocations reduces dislocation mobility due to dislocation interaction and entanglement. 20

Strengthening mechanisms F CC BCC H CP Face-centered B ody-centered Hexagonal Cubic Cubic close-packed A luminum I ron Titanium 12 S lip s ys tems 48 S lp s ystems 3 S lip s ys tems Slip system limitations lead to additional strengthening in polycrystalline metals 21

Strengthening mechanisms σ y = M τ y M = 3.02 (FCC ), M = 2.75 (BCC ) Polycrystalline metals require at least 5 independent slip systems. Thus grain boundaries and accommodation strains elevate the yield strength of polycrystals above that of single crystals 22

Strengthening mechanisms Dislocation pile-up at grain boundary σ y obstacle = σ i + k D 1/ 2 Hall-Petch relationship Flow stress for a poly-crystalline solid σ y = σ Pieierls + ( σ ss + σ dispersion + σ hardening )+ k D 1/ 2 σ y polycrystal = σ thermal + σ structural + k D 1/ 2 23

Aluminum fatigue limit Fatigue strength correlates with UTS and small grain size. 24

Influence of UTS and notches The fatigue limit of steel is a function of the UTS. However, stress concentrations resulting from either mechanical notches or corrosion pits greatly reduce the fatigue strength in proportion to the severity of the notch. 25