mohr circle1
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ManufacturingProcesses-MFRG315-Mohr'sCircle
1Introduction
Intwodimensionalstressanalysis planestress thereisofteninformationavailableaboutdirect sigmaxandsigmay andshearstresses tauxy actingonaparticularplaneandeither
thevaluesofthedirectandshearstressesactingonaplaneinclinedatsomeangletothefirstplanearerequired,oralternativelythevaluesofthe2principalstresses sigma1andsigma2
andtheinclinationoftheplaneonwhichtheyactarerequired.
Thistransformationcalculationcanbecarriedoutusingequations,butitwasnoticedbyMohrthatthesetransformationequationscanbecombinedtogivetheequationofacircle.Thisenablesthetransformationtobecarriedoutgraphically andtheequationsneednotberemembered .Usingthegraphicalconstructionalsomakesiteasiertovisualisealternative
scenarios.
InaMohrstresscircle,directstressesareonthehorizontalaxisandshearstressesareontheverticalaxis.RotationsofdirectioninaMohrcirclearedoublethoseintherealstressdistribution.Tensilestressesandashearstresstendingtocauseclockwiserotationaredeemedtobepositive.Compressivestressesandshearstressestendingtocausecounter-clockwiserotationaredeemedtobenegative.
Manymetalformingoperationsinvolvea3dimensionalstateofstresssothisisconsideredbelow.
2Mohr'sCircleforThreeDimensionalStatesofStress AgeneralapproachtoMohr'scirclein3dimensionsiscomplicated,howeverthisishardlyeverrequiredasinvirtuallyallmetalformingproblemsweknowthedirectionsofatleast1of the3principalstresses.
Ifthedirectionof1principalstressisknown,saysigma3,thenwecanimaginelookingback
alongthedirectionofsigma3totheplaneonwhichitacts asthisisaprincipalplanethere
arenoshearstressesactingonit andforthestressesactinginthisplanea2dimensionalMohr'scirclecanbeconstructedtodeterminethevaluesanddirectionsofthetwoprincipalstressesactinginit.
Giventhe3principalstresses,threecirclescanbeplotted,oneforeachprincipalplane.Wecandeterminethestressstatewithinaprincipalplaneaswerotateabouttheprincipalstressdirectionnormaltotheplane.Itisnotpossibleusingthisapproachtoconsidersimultaneousrotationsabout2ormoreprincipalaxes.
Itcanbestatedthat:Thestressesonanyplaneatanyrotation,whenplottedinthe3dimensionalMohr'scirclediagramwillberepresentedbyapointeitherononeofthe3circles,orwithinthe shaded areabetweenthelargestand2smallercircles.
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Themaximumshearstressisgivenbytheradiusofthelargestcircle.
SomesketchesofMohrcircleforcommonstressstatesareshownbelow:
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DeterminingtheStressStateonAnotherPlane Afurthergraphicalconstructionenablesthestateofstressonanyplanewhosenormalisinclinedatangles'alpha','beta'and'gamma'tothesigma1,sigma2andsigma3directions
respectivelytobedetermined. Withdirectioncosinestotheprincipalaxesdirections:l,mandn,respectively-Forinformationaboutdirectioncosines .
http://www.tech.plym.ac.uk/sme/mfrg315/dircos.gif
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Thefullprocedureis:
1.Drawthedirectstress horizontal andtheshearstress vertical axes.2.Markthethreeprincipalstressesonthehorizontalaxis,sigma1greaterthan
sigma2greaterthansigma3.
3.Drawthe3circles4.Drawthelinesigma1-A-Binclinedatanglealphafromtheverticalthroughsigma1.5.Drawthelinessigma2-Candsigma2-Dwithinclinationsofbeta,eithersideofthe
verticalthroughsigma2.
6.WithcentresC13andC23drawarcsDCandAB
7.ThedirectandshearstressatParegivenbyitscoordinates.
Anexamplecalculationisshowninthediagrambelow:
The3circlesaredrawnforthreeprincipalstresses:
sigma1=120MPa
sigma2=80MPa
sigma3=20MPa.
Thisgivesamaximumshearstressof50MPa.
Theconstructionshowsthedeterminationofdirectandshearstressesonaplaneat45oto
thesigma1directionand60otothesigma2direction point'P'onthediagram .Fromthescale
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diagramthedirectstressvaluevalueisabout87MPaandtheshearstressvalueisabout39MPa seebelow .
Thiscanbecheckedusingtheequations:
Firstdeterminethethirddirectioncosine:n= 1- l2+m2 0.5
n= 1- 0.70712+0.52 0.5=0.5
sigma=sigmall2+sigma2m
2+sigma3n2
sigma=120 0.7071 2+80 0.5 2+20 0.5 2=85MPa
Theshearstressisgivenby:
Shearstress2= sigma1l 2+ sigma2m
2+sigma3n 2-sigma2
shearstress=7200+1600+100-7225=40.9MPa.
Formostpurposesareasonablycarefulgraphicalconstructionprovidesadequateaccuracy