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Chapter3Materialmodelandmaterialcharacterizationofautomotivealuminiumalloy5052H34
3.1preface
Thebasicpropertyofmaterialdecidestheusefunctionofthestructure.intheresearchofcarcrashesandlargedeformationofkeycomponents,thekeypointofsolvingtheproblemistobuildcorrespondingphysics-mathmodelinordertoacquirethespecificmaterialparameters.Asfortheautomotivealuminiumalloyinourresearch,weneedtoconsidertheresponsecharacteristicofthematerialmachanismonconditionofrealimpact(suchasdynamicloading,high-stresscondition,includingprimarydefectsordamage,etc).Bythisway,numerousperformancetestandfull-sizecomponnetcrashtestneedtobeconducted,whichwouldexhaustgreatlaborpowerandphysicalresources,buttheresultisstilldubious.Withthelimiteddiscretdataobtainbytheexperiment,itcanhardlycoverthespaceofallsolutionofthemodel.Forsomeextremeconditionsuchasshearingstresscondtion,highstrainrate(ε-1≥2×
102),ithardtopredictitsmachanismresponse.Therefore,thismodelwebuilthasitscomparativelylargelimitations.Butcombinewithnumericalsimulations,itcanexpandthespaceofthemodeleffectively,whileobtaincompletematerialparameters.
Theresultshowsthattheprecisionofnumericalsimulationislargelydependontheprecisionofmaterialparametertoinput.Intheanalysisoflargedeformation,mater
-ialmachanismmustdescribethematerialchangefromelasticdeformation,elastoplasticdeformation,damageprogession,evolvement,fracture,whichismulti-stepmachanismprocedure.Besides,variousstrainrate,anisotropiccausedbyprocessinghistory,etcneedtobetakeintoaccounttoconsideritsaffectionwithconstitutiverelations.Previously,thisisaextremelycomplexproject,wheremanyproblemsisstillunsolved.J.G.BlauelandD.Z.Su,etcsimplyusedtensilebarexperimentcombinedwithfiniteelementtosimulatethecharacterizationofAW6016automotivealuminiumalloyandcrashtestofthetypicalcomponentsinautomobiles.Itpredictsthestaticanddynamicresponseofthealuminiumalloyandkeycomponentsinmacroperspective,andexpandG-T-Nmodelinmicroperspective,whichexplaintheductilefractureofthealuminiumanditsinitiationandevlovementbymachanismofgrowthofvoids,thatcouldbeappliedinengneeringcalculations.FranckLauroandBrunoBennanibuiltdynamicalloadingmachanismmodelonfinite-elementcalculationterrace.Thismodeltakeelasticflowandanisotropicofmicroholes’damageevolvementintoaccount.Therebythiscouldbeusedtopredictsituationofdamageandfractureofmaterialswithobvioustexturedeformationsuchasextrudedaluminiumalloysincircumstancesofdynamicloadingwithlargedeformation.TheotheronecontributionofFrank’sresearchistodevelopiterativealgorithmwhichisaexperimentcombinewithnumericalsimulationtoachievesolvingandcorrectthekeyparameterinmaterialmodel.Thismethodusesnotchtensiledataasthebasicinput,whichcanderiveparameterofG-T-Ndamagemodel,andrevisetheseparametersinconsiderofanisotropicfactors.Eventually,theresultofnumericalsimulationhitoffwithexperiments.Incomparewithothermaterialcharacterizationmethod,thiscouldavoidagreatamountofexperimentexpenses,andimprovingtheefficencyofmodelingrate.Ontheotherhand,thismethoddoesnotconsiderthechangesofdamagemachanismofthematerialsunderlowerstresscondition.Theresultprovedthatwhenthreedimensionstressdegreeisbelow1,withthereducingofstressdegree,shearslipfailurewouldtakethedominentposition,anddamageofvoidtypewillbesupressed.So,toadoptesingledamgemodelwouldlimititsapplicability.
Thischapteristryingtoconductmaterialcharacterization,acquirefractureparameterofthematerialundersimpletension,notchandshearstress,tocarryouttensiletestinconditionofstatic,quasi-staticanddynamicloading,andnumericalsimulation,furthermore,gainmachanicalpropertyunderdifferentstrainrate.Twokindsofdamagemodelwerebuiltinthisbasis,comparetheprecisionofmodelandsphereofapplicationofthesetwo,todescribethedamageandfracturebehaviourinlargedeformationfrommacrophenomenonanmicromachanism.
3.2Researchofmachanicalpropertytestofmaterialunderstaticanddynamicloading.
3.2.1Basicintroductionoftheexperiment
1.overallthinkingoftheexperiments.
Asfortheautomotivealminiumalloy5052H3.4,itismainlyusedinweldproductioninbearingweightcomponentofcar-body,inactualcollisiondesign,thesestructurewouldmostlyhavelargeelasticdeformationbeforefailure.Therefore,it’snotenoughformaterialcharacterizationonlyconsideringtosatisfystrengthdemand,therheologicalfutureofmaterialinlargeelasticdeformation,suchasworkhardening,anisotropicandfacturefeaturesofprimarydamageandevolvement,etc.Whilethesemachnicalpropertiesaretiedupwithinsidefactorssuchasmicrostruture,distribution,andoutsidefactorsofworkingtemperature,loadingrateandstresscondition.Asforspecificaluminiumalloy,itsorganizationstructureisfixed,buttheworktemperatureandloadingconditionvarieswiththeactualimpactprocess,soweneedtoconductaseriesofsysmaticalexperimentsoncharacterizationofthiskindofaluminiumalloy.Takeresearchinmachanicalresponseunderstaticanddynamiccondition.Onthissense,thisisaproject,whichneedsparticularcategoryandunifyrequirements.
2.Basicinformationofspecimens
Inaccordancewiththeactualimpactcondition,weneedtotakestaticanddynamicloadingmachanicalpropertytestinaluminiumalloy5052H43,theexperimentwasdividedintofivegroups,whichissmoothtensiletest,notchtensiletest,doublenotchsheartest,Iosipescusheartest,dynamictensileloadingtest.SerialnumberofthetestspecimensandexperimentconditionareshowinTable.3.1,sizesofthespecimensareshowinFig.3.2,thespecimensarecutfromoriginalplatebyusing(电火花技术),thedistributionofallthespecimensonplatecanbeseenonFig3.1.Asfortheserialnumberofthespecimens,takingPT1-UT-S1Qasanexampleforexplanation:
3.2.2Staticuniaxialtesniletest
3.2.2.1experimentequipment
Uniaxialsmoothtensiletestisoneofthebasicmachanicalpropertytest,whichismainlyusedtomeasureflowcurveofmaterialandstrengthindex.Theprimaryaimofthistestistomeasuretheactualstress-straincurveandfractureparameter,inordertoprovidewithmaterialpropertyforfollowingnumericalsimulation.Soastoexpandthescaleofthetestdata,obtainpracticaldataasmuchaspossible,theexperimentadoptedtwosetsofequipments.oneisthestrength-displacementdetectsystem,whichusesextend-measurementdisplacement,alsoloadingsensortomeasureload,whichisownedbyInstron1886tensiletestmachine.
Anothersetofmachineisopticaldeformationmeasuresystem,includingstaticcamera,digitaltransitioncardandfollowingimageprocessingsoftwareanddiagramcalculationsofteware.Thesystemisequipedwithtwosetsofdigitalcamera,theshootingangleisseperativelyperpendiculartofrontsideandlateralsideofthespecimens,distributtedby90degrees.Thereforeitcoulddetectchangesinwidthandthicknessdirectionimmediatelywhenthespecimenisinthetensileprocess,withdynamicimagedetectingtoacquirechangesinspecimensection,sowecouldcalculatetheminiumsectionsizeAi,accordingtotheformulationinfigure3.2tocalculatetheactualstress,strainintensileprocess,whichcouldgetstress-strainrelationofthetensilespecimensafternecking.Fig3.3istheschematicchartoftheexperimentequipments.Thesetwosetsofequipmentsworkscollaboratively.Thecommonstress-displcementismainlyresponsibleforrecordingofwholecourseloadingdetectionandelasticdeformationandpartialductiledeformation(beforemaxmiumloading),whiletheopticaldetectingsystemaimatrecordingofdetectionofelasticandductile(beforefracture)deformation.
WecanseefromChaper2.3.3thatthetruestrainofaluminiumalloy5052H34is9.6%correspondtostaticmaxmiumtensileloadatroomtemperature,andfracturestrainεfis73%atfracturing,atthistime,thesedatasegementisundetectablebyusingordinarytensileexperiment,andtherewillbesevereerrorinthecomingupnumericalsimulation.Bycontrast,segmentdataafterneckingcanberepairedifopticaldetectingsystemisused,andthemaxmiumtruestraincanbemeasuredupto56.1%.Themeasureproblemofstress-straincurvecanbefixedbylinearinterpolation.ComparisonofCurvesofspecificmaterialsandprecisionofnumericalsimulationwillbediscussedinthischapterinrelateddiagrams.
3.2.2.2Discussion
1Relationshipsofstress-strain
ThetruecurvesbytwosetsofdifferentkindsofdetectingsystemcanbeshowinFig3.4,wecanseethatthedatascaleofoptialdeformationsystemcoveredwider,whilethecomplexityandcostsofthisdetectingsystemisrelativelyhigher.
2Materialcharacterizationofrelativityofanisotropicandstresscondition
Specimenofsmoothtensiletestiscutfromthedirectionofverticalandparalleltotherollingdirection,theengineeringstress-striancurvescanbeseeninFig.3.5.Fromtheresult,theexperimentdisplayedexcellentrepitivenessandstablityofdatarecording.Curvesreactthatverticalyeildstressis22Mpahigherthanparallelyieldstress,tensilestrengthis26Mpahigher,whichdemostratesparticularanisotropic.Thesizeanddistributionofgrainsisregularfromfurtherresearchinmicrostructure.First,griansizesofthesufaceislargerthancentergrains(Fig.3.6).sec
-ondly,therearecertaingrainorientationinthecenterofthematerial(Fig.3.7).Partofthegrainintheaxisalong