Griffith Theory of Brittle Fracture

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    Observedfracturestrengthisalwayslowerthantheoreticalcohesivestrength.

    Griffithexplainedthatthediscrepancyisduetotheinherentdefectsinbrittle

    materialsleadingtostressconcentrationimplies lowerthefracturestrengthofthematerials.

    Crackpropagationcriterion: Considerathroughthicknesscrackoflength2a,

    subjectedtoauniformtensilestress ,atinfinity.

    Crackpropagationoccurswhenthereleasedelastic

    strainenergyisatleastequaltotheenergyrequiredto

    generatenewcracksurface.

    Griffiththeoryofbrittle

    fracture:

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    Thestressrequiredtocreatethenewcracksurface isgivenasfollows:

    Inplanestraincondition,theequationbecomes:

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    TheGriffithequationisstronglydependentonthecracksizea,and

    satisfiesonlyideallybrittlematerialslikeglass.

    However,metalsarenotideallybrittleandnormallyfailwithcertain

    amountsofplasticdeformation,thefracturestressis increaseddueto

    bluntingofthecracktip.

    IrwinandOrowansuggestedGriffithsequationcanbeappliedtobrittle

    materialsundergoneplasticdeformationbeforefracturebyincludingthe

    plasticwork, p,intothetotalelasticsurfaceenergyrequiredtoextend

    thecrackwall,givingthemodifiedGriffithsequationasfollows:

    ModifiedGriffithequation

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    InmodeIfailureandplanestraincondition,therelationship

    betweenGICan KICcanbeshownbyanexpressionasfollows:

    WhereKIC isthecriticalstressintensityfactor

    ilure

    Stressintensityfactor

    Crack deformation

    mode.

    Fracture modes

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    ` StressintensityfactorKICcanbedescribedasfracturetoughness

    ofmaterials(materialresistancetocrackpropagation)underconditionsof:

    1)brittlefracture

    2)inthepresenceofasharpcrack

    3)undercriticaltensileloading

    Where` KIC isthecriticalstressintensityfactorfor planestrainconditionin

    mode failure.

    ` ac isthecriticalcracklengthinaninfiniteplate

    ` app istheappliedstress

    ` isaparameterdependentonspecimenandcrackgeometry

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    Kvaluesofvariouscrackgeometries:

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    FracturetoughnessofmaterialcanbedeterminedaccordingtoLEFManalysis

    1)KICfracturetoughness:

    workswellforveryhighstrengthmaterials.exhibitingbrittlefracture

    2) CracktipopeningdisplacementCTOD:

    Usedforlowerstrengthmaterials(o

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    ` KIC fracturetoughnessofmaterialisobtainedbydeterminingtheabilityof

    materialtowithstandtheloadinthepresenceofasharpcrackbefore

    failure.

    ` Fracturetoughnessisrequiredinthesystemofhighstrengthandlight

    weight,i.e.,highstrengthsteels,titaniumandaluminium alloys.

    KICfracturetoughness

    Fracture toughness How longthe existing crack will growuntil the specimen fails

    Flaw geometry anddesign of cylindricalpressure vessel

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    BCCstructuremetalsexperienceductiletobrittletransitionbehaviour

    whensubjectedtodecreasingtemperature,resultingfromastrongyield

    stressdependentontemperature.

    Ductiletobrittletransition

    behaviour

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    BCCmetalspossesslimitedslipsystemsavailableatlowtemperature,

    minimisingtheplasticdeformationduringthefractureprocess.

    Increasingtemperatureallowsmoreslipsystemstooperate,yieldinggeneralplasticdeformationtooccurpriortofailure.

    Theoryoftheductiletobrittletransition: Thecriterionforamaterialtochangeitsfracturebehaviourfromductile

    tobrittlemodeiswhentheyieldstressattheobservedtemperatureis

    largerthanthestressnecessaryforthegrowthofthemicrocrackindicated

    intheGriffiththeory.

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    Cottrellstudiedtheroleofparameters,whichinfluencetheductileto

    brittletransitionasfollows;

    i is thelatticeresistancetodislocationmovement

    kisaparameterrelatedtothereleaseofdislocationintoapileup Disthegraindiameter(associatedwithsliplength).

    Gistheshearmodulus

    isaconstantdependingonthestresssystem.