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1、1附錄附錄A外文文獻(xiàn)外文文獻(xiàn)EffectsofgeometryfilletradiusondiestressesinstampingprocessesAbstract:Thispaperdescribestheuseofthefiniteelementmethodtoanalyzethefailureofdiesinstampingprocesses.Fthedieanalyzedinthepresentproblemthecracks
2、atdifferentlocationscanbeattributedtoacoupleofmechanisms.Oneofthemisduetolargeprincipalstressestheotheroneisduetolargeshearstresses.Athreedimensionalmodelisusedtosimulatetheseproblemsfirst.Themodelisthensimplifiedtoanaxi
3、symmetricproblemfanalyzingtheeffectsofgeometryfilletradiusondiestresses.2000ElsevierScienceS.A.Allrightsreserved.Keywds:StampingMetalfmingFiniteelementmethodDiefailure1.IntroductionInmetalfmingprocessesdiefailureanalysis
4、isoneofthemostimptantproblems.Befethebeginningofthisdecademostresearchfocusedonthedevelopmentoftheeticalnumericalmethods.Upperboundtechniques[12]contactimpactprocedures[3]thefiniteelementmethod(FEM)[45]arethemaintechniqu
5、esfanalyzingstampingproblems.WiththedevelopmentofcomputertechnologytheFEMbecomesthedominanttechnique[612].Altancowkers[1314]discussedthecausesoffailureinfgingtoolingpresentedafatigueanalysisconceptthatcanbeappliedduringp
6、rocesstooldesigntoanalyzethestressesintools.Inthesetwopaperstheyusedthepunchingloadastheboundaryfcetoanalyzethestressstatesthatexistinthesduringthefmingprocessdeterminedthecausesofthefailures.Basedontheseconceptstheyalso
7、gavesomesuggestionstoimprovediedesign.Inthispaperlinearstressanalysisofathreedimensional(3D)diemodelispresented.Thestresspatternsarethenanalyzedtoexplainthecausesofthecrackinitiation.Somesuggestionsaboutoptimizationofthe
8、dietoreducethestressconcentrationarepresented.Indertooptimizethedesignofthedietheeffectsofgeometryfilletradiusarediscussedbasedonasimplifiedaxisymmetricmodel.2.Problemdefinition3FthetwomeshesusedinCase1.Themaximumprincip
9、alshearstress(S12)distributionattheregionoffilletareshowninFig.4ab.Theresultsshowthatthestressdistributionpatternsarethesamefthetwodifferentmeshestherefetheconvergenceofthesolutionsisestablished.Altancowkers[14]haveprese
10、ntedthestressanalysisofanaxisymmetricupperdie.Intheirwkwhenthematerialofthewkpieceflowstofillthevolumebetweenthediescollarthecontactsurfaceofthedieisstretched.Attheareaofthetransitionradiustheprincipalstresseschangedirec
11、tionreachhightensilevalues.Accdingtotheiranalysisthefatiguefailureisduetotwofacts:(i)whenthestressexceedstheyieldstrengthofthediematerialalocalizedplasticzonegenerallyfmsduringthefirstloadcycleundergoesplasticcyclingduri
12、ngsubsequentunloadingreloadingthusmicroscopiccracksinitiate(ii)tensileprincipalstressescausethemicroscopiccrackstogrowleadtothesubsequentpropagationofthecracks.TheVonMisesstressdistributionisshowninFig.5a.Veryhighstresso
13、ccurinthehalfmoonfilletregions.Ifthecontactpressurekeepsincreasingplasticzoneswillfmfirstinthesetworegions.Fig.5bshowsthemaximumprincipalstress(SP3)distributionpattern.IndertoshowtheareaofCrackIinitiationFig.5cprovidesaz
14、oomedviewofthearea.Itisclearthatatensileprincipalstress(SP3)concentrationof25.5MPaexistsbetweenthehalfmoonpatternthefreeedgeisthecauseofcrackinitiation.SinceCrackIpropagatesnearlynmaltothe12planethedirectionofthestresses
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