Fracture Mechanics Lecture Slides.pptx

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    DR MARK BINGLEY

    PEMBROKE 237

    [email protected]

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    MECH 1064

    APPLIED ENGINEERING MECHANICS

    3 SUBJECT AREAS

    MECHANICS OF MATERIALS Mark BingleyMECHANICS ` Michael OkerekeENGINEERING DYNAMICS Kaushika Hettiartachi

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    MECHANICS OF MATERIALS IN CONTEXT

    Engineering Mechanics is concerned with analysing stresses in abody or component subject to external loading

    Stress analysis deals with:

    Tension/Compression LoadsTorsionBending

    MECHANICS OF MATERIALS assesses whether theresultant stresses in a body are large enough to causefailure

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    FAILUREFAILURE is said to occur if the stresses causes changes in thecomponent that mean it is no longer fit for use(it does not necessarily mean catastrophic fracture - separation of abody into 2 or more parts although it could)

    TYPES OF FAILURE - EXAMPLES

    Yielding and Plastic DeformationDuctile FractureBrittle Fracture

    FatigueCreep Deformation and FailureComposite FailureWear

    Corrosion

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    FRACTURE MECHANICSFast, Unstable, Catastrophic

    BRITTLE FRACTURE

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    This is an exampleof brittle fracturecaused by usingcold water for ahydrostaticpressure test andthen pressurizingvessel. Thetemperature of the

    water caused themetal to becomebrittle.

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    Jan. 15, 1919: Morass of Molasses Mucks Up Boston

    21 dead - 150 injuredImage below shows elevated train structure destroyed in incident

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    AIMS AND OBJECTIVES OF LECTURE To appreciate which materials are susceptible

    to Brittle Fracture

    To understand the role of cracks in BrittleFracture

    To understand the concepts of FractureMechanics through a stress analysis approach

    To be able to analyse simple problems inFracture Mechanics and carry out thecalculations necessary to solve problems

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    TENSILE BEHAVIOUR OF CERAMICS(TYPICAL BRITTLE MATERIALS)

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    WHY CONCRETE IS BRITTLE

    http://www.bbc.co.uk/learningzone/clips/13763.flv

    http://www.bbc.co.uk/learningzone/clips/13763.flvhttp://www.bbc.co.uk/learningzone/clips/13763.flvhttp://www.bbc.co.uk/learningzone/clips/13763.flvhttp://www.bbc.co.uk/learningzone/clips/13763.flv
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    TENSILE BEHAVIOUR OF HIGH STRENGTHMETALS

    NORMAL DUCTILE BEHAVIOUR BRITTLE BEHAVIOUR

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    WHICH MATERIALS ARE SUSCEPTIBLE TOBRITTLE FRACTURE

    HIGH STRENGTHLOW-DUCTILITY MATERIALS:

    CERAMICS AND GLASSES

    HIGH STRENGTH METALS Low C Steels (at low

    temps) Medium-High C Steels

    Q and T Steels Aerospace/Automotive

    Al Alloys Titanium Alloys

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    TOUGHNESSTHE RESISTANCE TO FRACTURE

    TOUGH MATERIALS

    Require large amounts of (Deformation) Energyto cause Fracture

    BRITTLE MATERIALSFail with low Energy input

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    IMPACT TESTING

    final height initial height

    Impact loading:

    -- severe testing case-- makes material more brittle-- decreases toughness

    Adapted from Fig. 8.12(b),Callister 7e. (Fig. 8.12(b) isadapted from H.W. Hayden,W.G. Moffatt, and J. Wulff, TheStructure and Properties ofMaterials , Vol. III, MechanicalBehavior , John Wiley and Sons,Inc. (1965) p. 13.)

    (Charpy)

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    Increasing temperature...

    --increases % EL and K c Ductile-to-Brittle Transition Temperature (DBTT) ...

    TEMPERATURE

    BCC metals (e.g., iron at T < 914 C)

    I m p a c

    t E n e r g y

    Temperature

    High strength materials ( y > E /150)

    polymers

    More DuctileBrittle

    Ductile-to-brittletransition temperature

    FCC metals (e.g., Cu, Ni)

    Adapted from Fig. 8.15,Callister 7e.

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    IMPORTANCE OF CRACKSCRACKS OR FLAWS MUST BE PRESENT FOR BRITTLE FRACTURE TO

    OCCUR

    In inherently brittle materials such as ceramics the cracks may besub-microscopic

    However Larger Cracks Form Easily in Metals During Casting

    During Forming During Heat-Treatment During Grinding During Joining (WELDING) During Service (Corrosion, Wear, Mishandling, Fatigue)

    QUESTION WE NEED TO ASK:UNDER WHAT CIRCUMSTANCES (LOAD CONDITIONS) DO CRACKSPROPAGATE?

    This is the area of FRACTURE MECHANICS

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    STRESS ANALYSIS OF CRACKS(LOADING MODES)

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    STRESS ANALYSIS OF CRACKS(MODE 1 LOADING)

    CRACKS ARE DANGEROUSBECAUSE:

    THEY ACT AS STRESSRAISERS

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    Linesrepresentareas of equalstress

    Where linesare closetogether is anarea of stress

    concentration

    STRESS CONCENTRATION IN PERSPEX UNDER LOADING

    All specimens are ofequal width at theircentre abruptchanges in cross-section give rise tolarger stressconcentrations

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    HOW DANGEROUS (HOW LIKELY TOCAUSE FAILURE) A CRACK IS,

    IS DETERMINED BY SOMETHINGCALLED THESTRESS INTENSITY FACTOR

    THE SIZE OF THE STRESS INTENSITYFACTOR IS RELATED TO:

    THE STRESS ON THE CRACKEDCOMPONENT THE SIZE OF THE CRACK

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    STRESS INTENSITY FACTOR (K)

    K = APPLIED Stress Intensity Factor

    Magnitude of K depends upon:Applied Stress( )Crack Length (a)Crack Shape Factor (Y)

    Y depends uponCrack shapeSpecimen size, shapeGeometry and type of loading

    aY K s

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    STRESS INTENSITY FACTORK

    This is a measure of the intensity of the localstress at the crack rootAs will be seen on the following slides it varies withthe geometry of the part

    Figs (a), (b), (i), (j) represent infinite (large) plates plate dimension >>> crack length

    Figs (c), (d), (f), (g) represent finite platesplate dimension crack length

    STRESS INTENSITY

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    STRESS INTENSITYFACTOR SOLUTIONS

    (a), (b)Infinite (large) Plates)

    a K b

    a K a

    s

    s

    1.1)(

    )(

    (c)Finite Plates

    Y varies with 2 a /W ratioAccording to graphical solutions

    1.1 = edge factor

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    STRESS INTENSITY FACTOR SOLUTIONS CONT`D

    (d), (e)Finite Plates Y varies according to graphs

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    STRESS INTENSITY FACTOR SOLUTIONS

    Y value indicated for a/W = 0.4

    (f), (g)Finite Plates Y varies according to graphs

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    STRESS INTENSITY FACTOR SOLUTIONS CONT`D

    Solutions for

    (i) Circular cracks(j) Elliptical cracksembedded in

    infinite (large)plates

    NOTE:For Semi-circularand Semi-ellipticalcracks at thesurface/edge of aplateThe equationsgiven are multipliedby the edge-factor(1.1)

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    STRESS INTENSITY FACTORS CONT`DTo be used with the Elliptical Crack Solution (j)

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    FRACTURE

    FAST BRITTLE - FRACTURE WILL OCCUR WHEN:

    K = K IC

    KIC is the CRITICAL STRESS INTENSITY FACTORorPLANE STRAIN FRACTURE TOUGHNESS

    KIC is a MATERIAL PROPERTY

    IC K aY s

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    FRACTURE TOUGHNESS VALUES OF A RANGE OFMATERIALS

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    FRACTURE STRESSAt Fracture:

    Applied Stress ( ) = Fracture Stress ( f )

    IMPORTANTFracture Stress of a material is not ConstantIt depends on the crack length present

    Large Crack Length gives Low Fracture StressSmall Crack Length gives High Fracture Stress

    aY K f IC s

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    UNITS OF K AND KICK = Y a

    K = (MPa)(m) = MPam

    K = (MN/m 2)(m 1/2 ) = MNm -3/2

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    CLASS EXAMPLES1. A plate is to be loaded in service to a stress of 400 MPa.

    Examination of the plate reveals a centre crack 10 mm long.If the plane strain fracture toughness (K 1C) is 70 MPam , isthe plate safe to be put into service?

    2. A plate was found to contain a circular shaped crack 15 mmin diameter. The plate fractured at a stress of 650 MPa.What is the K 1C value of the material ?

    3. An aerospace aluminium alloy has a yield stress of 500 MPaand a plane strain fracture toughness value (K 1C) of

    25 MPam . The design stress is half the yield stress. What isthe critical crack size (that would result in fracture). Assumethat the crack is in the form of an edge crack.

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    Q1 ANSWER

    For centre-crack in infinite plate refer to fig 8.7(a)

    2a = 10 mm

    a = 5 mm

    K = 50.13 MPam

    K IC = 70 MPam K < K ICNO FRACTURE

    a K s

    3105400 K

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    Q2 ANSWER

    Circular crack in infinite plate refer to fig 8.7(i)

    2a = 15 mm

    a = 7.5 mm

    K IC = 63.5 MPam

    a K s

    2

    3105.76502

    IC K

    a K f IC s

    2

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    Q3 ANSWER

    Edge crack in infinite plate refer to fig 8.7 (b)

    Assume design stress = fracture stress = f = ( y / 2)Where y = yield stress

    Critical crack size ( a ) = 0.0026 m = 2.6 mm

    a K s 1.1

    a K f IC s 1.1

    a 2

    5001.125