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Denand, B. and Esin, V.A. and Dehmas, M.
and Geandier, G. and Denis, S. and Sourmail, T. and Aeby-Gautier,
E.
Carbon content evolution in austenite during austenitization
studied by in situ synchrotron X-ray diffraction of a hypoeutectoid
steel.
(2020) Materialia, 10. 100664. ISSN 25891529
Full Length Article
Carbon
content
evolution
in
austenite
during
austenitization
studied
by
in
situ
synchrotron
X-ray
diffraction
of
a
hypoeutectoid
steel
B. Denand
a,c,∗, V.A. Esin
b, M. Dehmas
d, G. Geandier
a,c, S. Denis
a,c, T. Sourmail
e,
E. Aeby-Gautier
a,caInstitutJeanLamour,UMR7198CNRS,Université deLorraine,Nancy,France
bMINESParisTech,PSLUniversity,CentredesMatériaux(CMAT),UMR7633CNRS,Evry,France
cLaboratoryofExcellenceforDesignofAlloyMetalsforLow-massStructures(‘DAMAS’Labex),Université deLorraine,France dCIRIMAT,Université deToulouse,CNRS,Toulouse,France
eAscometal-CREAS(ResearchCentre),Hagondange,France
a
r
t
i
c
l
e
i
n
f
o
Keywords:Austenitization
InsitusynchrotronX-raydiffraction Latticeparameter
Carboncontent Thermo-Calc
a
b
s
t
r
a
c
t
UsinginsituhighenergyX-raydiffractionstudyofausteniteformationinhypoeutectoidsteelwiththree differ-entinitialmicrostructures(ferrite-pearlite,temperedmartensiteandbainite),thelatticeparametersofferrite, cementiteandausteniteareexaminedonheatingat0.25,10and100°C/s.
Thelatticeparametersofferrite,cementiteandaustenitedonotvarylinearlywiththetemperature,especially, inthetemperaturerangewheretheaustenitizationtakesplace.Fortheaustenite,itissuggestedthatthedeviation fromthelinearityismainlyassociatedtothecarboncontentvariation.UsingDysonandHolmesequation,the carboncontentinausteniteisevaluatedforanymomentoftheausteniteformationforeachinitialmicrostructure andallheatingrates.
Fortheferrite-pearlitemicrostructureheatedat0.25°C/s,thecarboncontentinausteniteaftercomplete cementitedissolutioncorrespondstothatofpearlite.Moreover,arapiddecreaseincarboncontentintheaustenite isobservedduringthefirststageoftheaustenitization(simultaneousdissolutionofferriteandcementite)followed byaslowfurtherdecreaseduringthetransformationoftheremainingferrite.Theobtainedresultsarediscussed usingthermodynamiccalculations.
1. Introduction
Theservicelifeofcrankshaftsforautomotive industrycan be in-creasedbysurfacehardeningvia aninduction heattreatment [1,2]. Suchalocalheattreatmentleadstoaformationofaustenitecloseto thesurfacewhichfurthertransformsintomartensiteuponsubsequent quenching.Therefore,theresultingsurfacelayerhasahigherhardness incomparisonwiththatofthebulk.Inaddition,retainedcompressive stressesaregeneratedinthesurfacelayer(mainlyduetothemartensitic transformationinthatarea),optimalforthepropertiesofcrankshafts use[3].
Therequiredheattreatmentshouldbefastenoughtolimitthe vol-umeofthematerialtransformedintoaustenite(closetothesurface)on heating.Typicalheatingratesvaryfrom30toover100°C/s.Inthese conditions,theinitialmicrostructureofthesteelmayaffectthe austeni-tizationkineticsduetodifferencesininterfacemigrationandinterstitial andsubstitutionalelementsredistributionindifferentmicrostructures. Evenforafullyausteniticlayer,thechemicalcompositionmaypresent localheterogeneitiesduetoinitialmicrostructurefeaturesleadingthus
tolocaldifferencesinfinalmicrostructurewithdifferentlocal mechani-calproperties.Itisworthnoting,thatmostofinvestigationsreportedin literaturehavebeencarriedoutontheaustenitizationofsteelswith ini-tialferrite-pearlitemicrostructure[4–14].Theanalysisofaustenite for-mationforthesamesteelhavingdifferentinitialmicrostructuresandfor differentheatingratesisoftechnologicalandfundamentalimportance. Inthis scope,ourprevious studyreportedon thekineticsof austen-iteformationconsideringthreeinitialmicrostructures(ferrite-pearlite, temperedmartensiteandbainite)ofthesamehypoeutectoidsteeland fiveheatingrates(0.25,1,10,60and100°C/s)[15].TheuseofHigh EnergysynchrotronX-RayDiffraction(HE-XRD)[16]allowedto char-acterizethephasefractionevolutionofallphasesandhighlightedtwo stepsintheausteniteformation[15]:(i)thesimultaneous transforma-tionofferriteandcementiteintoaustenite,and(ii)thetransformationof theremainingferriteintoaustenite.Foragivenheatingrate,thekinetics ofeachstepwasshowntobedependentontheinitialmicrostructure.
Inadditiontothenatureandamountofphasesformed,theRietveld refinementofdiffractionpatternsgivesalsoinformationaboutthe lat-ticeparametersandwidthsofdiffractionspeaksfordifferentphasesfor
∗Correspondingauthorat:InstitutJeanLamour,UniversitédeLorraine,CNRS,UMR7198,54011NancyCedex,France.
Table 1
Chemicalcomposition(wt.%)ofthe37MnCr4-3steelused.
Fe C Si Mn S Ni Cr V Mo Cu Al
Bal. 0.356 0.253 1.285 0.024 0.208 0.652 0.005 0.065 0.172 0.018
anymomentduringheatingandtheausteniteformation.Togetinsight intothetransformationfeatures,thepresentpaperfocusesonthe evo-lutionoflatticeparametersofaustenite,ferriteandcementitetobeable toestimatethecarboncontentevolutionsinthephases.
It is worth noting that a recent studyattempted to analyze the evolutionof austenitelatticeparameterduringaustenitizationof the same50CrMo4steelhavingferrite-pearliteandsoftannealedinitial mi-crostructuresclosetoequilibriumstate[14].InsituHE-XRDwasused onheatingwiththeratesof1,10and100°C/s.Adecreaseinaustenite latticeparameterwasobservedatthebeginningof theaustenite for-mationuntilaminimumvaluefollowedbyfurtherlinearincreasewith temperature.Suchachange inaustenitelatticeparameterwas quali-tativelyattributedtotheevolutionofaustenitechemicalcomposition. However,anyattemptwasnotdonetoquantifyaustenitecarbon con-tentorlatticeparameterevolutionofferritecementiteandaustenite, andonlypossibleexplanationsweregiven.
InthepresentworkanaccurateanalysisofX-raydataiscarriedout usingRietveldrefinement.Differentassumptionsconcerningthe evolu-tionoflatticeparametersofferrite,cementiteandausteniteare care-fullyanalyzedtobeabletoobtaintheaustenitecarboncontentatany momentofthetransformationfordifferentheatingrates.Besides, non-equilibriumtemperedmartensiteandbainitemicrostructuresare inves-tigatedtogetherwithferrite-pearliteinitialmicrostructure.
2. Material
Thesteelusedinthepresentworkisa37MnCr4-3,whichwas man-ufacturedbyAscometalCREAS.Thechemicalcompositionwas charac-terizedonforgedbarsusingopticalemissionspectrometryand combus-tion(LECO)analysisforaccuratemeasurementsofcarbonandsulphur contents(Table1).Thesteelwasmadeavailableashotforgedbarsof approximatediameter40mm.Detailsofthefabricationprocesshave alreadybeenreportedin[15].
Toproducedifferentinitial microstructures,theforgedbarswere austenitizedat850 °Cfor1handfurthersubjectedtodifferentheat treatments.These thermal treatments have already been detailedin [15],butwillneverthelessbesummarizedforeaseoflegibility.To ob-tainferrite-pearliteinitialmicrostructure,thesteelwasaircooledfrom austenitizingtemperaturedownto625°Candheldatthistemperature for1h.Thetemperedmartensiterequiredoilquenchingatroom tem-peraturefromaustenitedomainfollowedbyatemperingat500°C dur-ing1h.Thebainitemicrostructurewasobtainedduringanisothermal soakinginasaltbathat450°Cduring30minafteraustenitizing.
Thesamplesusedinthisstudyweretakenatthemidradiusofthe barsforeachinitial microstructurein ordertoavoid decarburization phenomenonatthesurfaceofthesebars.Theseinitialmicrostructures obtainedbyScanningElectronMicroscopy(SEM)arepresentedinFig.1. Fig.1(a)showstheinitialferrite-pearlitemicrostructurewhereblack regionsarethefreeferriteandgreyregionsarethepearlite.Volume frac-tionofferriteandpearlitecanbedeterminedbyimageanalysisbased oncontrast threshold.Themeanphase fractionobtainedforthefree ferriteis20%andthatforthepearliteis80%.Theinterceptsmethod allowedustoestimatethesizeofmeanpro-eutectoidferritegrainsto beof10μm.Fortheinitialtemperedmartensiteandbainite microstruc-tures(Fig.1(b)and(c)),itwasnotpossibletodistinguishthedifferent phasesbySEM.
HE-XRDanalysisrevealedthepresenceofabout2–3wt.%of cemen-titeforthethreeinitialmicrostructuresand3wt.%ofretainedaustenite inthebainiticmicrostructure.
3. Experimentaltechniques
Experiments were carried out at the Deutsches Elektronen-Synchrotron(DESY,Hamburg,Germany)onthebeamlineP07 of PE-TRAIII.ADIL805A/DdilatometerfromTAInstrumentwasusedto ap-plythethermal treatments.Threelinearheatingrates (0.25,10 and 100°C/s)wereimposeduntil900°Cfollowedbygasquenching.
Thesampleswerehollowcylindersof10mmlengthwhosethe ex-ternaldiameterwas4mmandthethicknesswas0.5mminorderto reduceradialthermalgradient.
Induction heatingwasemployed duringtheexperiments and the temperaturewascontrolledusingS-typethermocouplecentrallywelded atthesurfaceofthehollowcylinder.Inordertohaveagood correla-tionbetweenthetemperatureacquisitionandtheDebye-Sherrerrings recordedduringthethermaltreatment,theX-raybeamcrossedthe sam-pleintheareaclosetothermocouple.TheDebye-Scherrerringswere ob-tainedbyusingamonochromaticbeamof100keVand2Dimageplate detectorsituatedatabout1.5mawayfromthesample.Apreliminary calibrationwithCeO2powderwascarriedouttodeterminethevalues
requiredforfurtherX-raydataanalysissuchasthedistancebetweenthe sampleandthedetectororthewavelengthwhichwas0.123984Å inthis case.Thebeamsizeof1.0×1.0mm2allowedgettingareasonablygood resolutionandfastacquisitiontimeforthehighheatingrates.Indeed, twomodeswereemployedtothediffractionpatternrecording:aslow modewithanacquisitiontimeof3.5sfortheheatingrateof0.25°C/s andafastmodewithanacquisitiontimeof0.1sfortheheatingratesof 10and100°C/s.Fortheslowmode,theacquisitiontimeincludedthe shutteropeningandclosing,theacquisitionofexternalparameterasthe temperature,andthedataerasingfromthedetector.Inthefastmode, theshutteropenedatthebeginningoftheexperimentandclosedatthe end;anyexternalparameterwasnotrecordedduringtheacquisition.
Thefastmodeledthustoanuncertaintyintemperaturevaluewhich canbecalculatedasΔ𝑇=±0.1 × 𝑉ℎ,whereVh(°C/s)istheheating rateand0.1(s)istheacquisitiontimeinfastmode.
Itisworthnotingthatforthepresentstudythreeheatingrateswere selected:0.25,10and100°C/swhile1and60°C/sheatingrateswere usedaswellinthestudyonaustenitizationkineticsinthesamesteelin [15].
TheDebye-Scherrer ringsgiveinformationonthesample crystal-lographyatanymomentduringthethermalpath.Thecomplete inte-grationoftheseringsleadingtoconventional1-Ddiffractogramswere madeusingtheFit2Dsoftware.Then,thediffractogramswereanalyzed byRietveldrefinement[17,18]withtheFullProfsoftware[19].
ThestartingstructuresfortheRietveldanalysisconsistedofferrite andcementitefortheinitialferrite-pearliteandtemperedmartensite microstructures,andofferrite,cementiteandaustenitefortheanalysis ofthebainiticmicrostructure.Moredetailsconcerningtheprocedureof Retvieldrefinementcanbefoundin[15]
ForeachXRDpattern,thefollowingparameterswererefined:scale factors,massfractions,FWHM(fullwidthathalfmaximum)andlattice parameters.
4. Results
Thekineticsofausteniteformationasfunctionofinitial microstruc-ture andheatingratewasreportedin detailsin[15].Werecallhere themainresultsandconclusionsrequiredforthefurtheranalysisofthe latticeparametersevolutions.
B.Denand,V.A.EsinandM.Dehmasetal.
Fig. 1. Initial(a)ferrite-pearlite,(b)bainiteand(c)temperedmartensitemicrostructuresoftheinvestigatedsteelasobservedbySEM(standardmetallography preparationand2%Nitaletching).
Table 2
Thetemperaturesofthestart(AC1)andend(AC3)ofausteniteformationonheatingaswellasthetemperatureoftheendofthefirststageofausteniteformation (T1)accordingtothedataobtainedfromHE-XRDexperimentsin[15]fordifferentinitialmicrostructuresandheatingrates.
Heatingrate(°C/s) Ferrite-pearlite Temperedmartensite Bainite
AC1(°C) T1(°C) AC3(°C) AC1(°C) T1(°C) AC3(°C) AC1(°C) T1(°C) AC3(°C)
0.25 740 753 790 736 758 774 736 763 770
10 761 792 822 743 763 779 741 769 790
100 781 843 854 753 788 810 743 789 810
Table 3
Volumecoefficientofthermalexpansionofcementiteinthetemperaturerangefrom450to600°C,andlinearcoefficientofthermalexpansionofferriteandaustenite inthetemperaturerangewherenotransformationoccurs.
Coefficientofthermalexpansion(10−6K−1) Initialmicrostructure Literaturedata
Ferrite– pearlite Bainite Temperedmartensite
Volume,cementite 54 56 54 46[25],58[26]
Linear,ferrite 16.4 16.2 16.1 14–16[20,21],16.3[23],16.8pureiron[23],16[25]
Linear,austenite 24.7 24.9 24.4 20–23[20],24[21]
Thetemperaturerangeofausteniteformationonheatingfor differ-entconditionsisgiveninTable2.Inordertoobtainagoodconfidence onthesetemperatures,thestartofaustenitization(AC1)istakenfora
massfractionof3%ofaustenitecreatedandtheferritedissolutionis consideredascompleted(AC3)for95%ofausteniteformation.
ThedatareportedinTable2clearlyevidencethatthe transforma-tionkineticsisdependingontheinitialmicrostructure,mainlythesize ofthedifferentmicrostructureconstituents[15].Thephasefraction evo-lutionsshowtwostagesinthekineticsofausteniteformation.Thefirst onecorrespondstothesimultaneousdissolutionofferriteand cemen-tite;thesecondonetothedissolutionoftheremainingferrite.The tem-peratureoftheendofthefirststage(T1)isrecalledinTable2.This
temperatureisdependentontheinitialmicrostructureandheatingrate anditsvariationwasattributedtodifferentsizeofcementiteparticles indifferentinitialmicrostructures[15].
Togetherwithphasefractions,theresultsofRietveldrefinement in-formaboutevolutionofthemeanlatticeparametersofferrite,cementite andaustenite.Thosearefurtheranalyzedanddiscussedconsideringthe differentoriginsoflatticeparameterevolution:thetemperature varia-tion,theelasticstrainsand/orthevariationofchemicalcompositionof differentphasesduringaustenitization.
4.1. Meanlatticeparametersonheating
Thevariationofmeanlatticeparametersofferriteandaustenite dur-ingheatingwitharateof0.25°C/sisgiveninFig.2forthethreeinitial microstructures.Forcementite,thechangeinunitcellvolumeon heat-ingisreportedinFig.3forthesameconditions.Thevaluesofapparent coefficientsofthermalexpansion,obtainedinthetemperatureranges
wherenotransformationoccurred,aresummarizedinTable3forall phases.1
Fortheferrite-pearliteandtemperedmartensiteinitial microstruc-turesthatcontainamixtureofferriteandcementite,themeanlattice parameterofferriteincreaseslinearlywithtemperatureupto735°C. Between735°Candaround760°C,inthefirststageoftheaustenite formation,themeanlatticeparameterofferriteslightlydeviatesfrom thelinearbehavior,withadecreaseintheapparentCoefficientof Ther-malExpansion(CTE).Above760°C(Fig.2(b)),inthesecondstageof thetransformation,thelatticeparameterofferritedecreaseswitha neg-ativeapparentCTE.Forbothferrite-pearliteandtemperedmartensite microstructures,theunit cellvolumeof cementiteincreaseswith in-creasingtemperature:alinearbehaviorisonlyobservedbetween450 and735°C(Fig.3).Above735°Cwherecementitedissolutionoccurs, adecreaseintheunitcellvolumeofcementiteisobserved.Forthe bai-nitemicrostructure,theinitialstatecontainsamixtureofthreephases (ferrite,cementiteandretainedaustenite).Duringtheheatingbetween 240and410°C,thetransformationofretainedausteniteintoferriteand cementiteoccurs.Between410and735°C,theamountofferriteand cementiteremainsconstant.Nevertheless,themeanlatticeparameters offerriteandcementitehavealmostasimilarevolutionthantheone obtainedforferrite-pearliteandtemperedmartensitemicrostructures.
1Thevolumethermalexpansioncoefficientsofcementiteweremeasuredin thetemperaturerange450–600°Cfortworeasons:(i)thesestemperaturesare higherthancementiteCurietemperature(Tc≈227°C)[20](magnetictransition hasasignificanteffectonthethermalexpansioncoefficientinatemperature rangeofabout200°CaroundTc);(ii)fortheinitialbainitemicrostructuresome transformationoftheretainedausteniteoccurredfortemperatureslowerthan 450°Candmayaffecttheapparentthermalcoefficientofcementite.
Fig. 2. Meanlatticeparametersofferriteandausteniteonheatingwithaheatingrateof0.25°C/sforinitialmicrostructuresofferrite-perlite(solid),bainite(dashed) andtemperedmartensite(dotted):(a)before,duringandafteraustenitizationand(b)zoomtothetemperaturerangewheretheausteniteformationoccurs.
Fig. 3. Unitcellvolumeofcementitebeforeandduringaustenitizationwitha heatingrateof0.25°C/sforinitialmicrostructuresofferrite-pearlite(blue), bai-nite(red)andtemperedmartensite(black).(Forinterpretationofthereferences tocolorinthisfigurelegend,thereaderisreferredtothewebversionofthis article.)
Fortheevolutionofaustenitelatticeparameter, twotemperature rangesshould bedistinguished:(i)above730°C whereamixture of ferriteandcementite transforms intoaustenite (ferrite-pearlite, tem-peredmartensiteandbainitemicrostructures),and(ii)between240and 410°Cwhereretainedaustenitetransformsintoferriteandcementite (bainitemicrostructureonly).
Acomplexnon-linearevolutionofaustenitelatticeparameterwith temperatureisobservedduringtheferrite+cementite→austenite trans-formationwhatevertheinitialmicrostructure(Fig.2(b)).Asignificant decreasein austenitelatticeparameteris observedbetween 735and 760°C,duringthefirststageofthetransformation.Above760°C, dur-ingthesecondstageofthetransformation,theaustenitelattice param-eterincreases.TheCTEofausteniteincreasesuntilreachingaconstant valueof25×10−6K−1oncethetransformationiscompleted.
Forinitialbainiticmicrostructure,theCTEofretainedaustenite ob-tainedbetweenroomtemperatureand240°Cisequalto21×10−6K−1
whichislowerthantheCTEmeasuredaftercompleteaustenitization, couldindicatethattheretainedausteniteisunderacompressivestress
state[27].Above240°C,theapparentCTEincreasesupto41×10−6K−1
wheretheretainedaustenitetransformsintoferriteandcementite. Inthetemperatureranges whereno transformationoccurred,the coefficientsofthermalexpansionobtainedfortheferrite,cementiteand austeniteareingoodagreementwiththosefoundinliterature(Table3, [20–26]).
Asimilarevolutionofferrite,cementiteandaustenitelattice parame-terswithtemperaturewasobservedforheatingratesof10and100°C/s forthedifferentinitialmicrostructuresasillustratedforferrite-pearlite microstructureinFig.4.
Thecomplexvariationsofmeanlatticeparametersofeachphasecan beduetoseveralfactors:changeintemperature(thermalexpansion), elasticstrainandchangeinchemicalcomposition.Asthetemperature wasmeasuredallalongtheexperimentandthermalgradientswere neg-ligible,thosevariationscanbefurtheranalyzedsubtractingthethermal contributionusingthedatareportedinTable3.
4.2. Ferriteandcementitelatticeparametersbeforethe ferrite+cementite→austenitetransformation
First,themeanlatticeparameterofferriteobtainedonheatingfor the threeinitial microstructuresis comparedwith thatof pureiron, heated on the same apparatusand in the same conditions (Fig. 5). Theabsolutevaluesofferritelatticeparameterforthethreeinitial mi-crostructuresareslightlydifferentandareslightlylowerascompared tothelatticeparameterofferriteinpureiron.Thosedifferencescanbe attributedtodifferencesinchemicalcompositionoftheferriteaswell astointernalstresses.
The differences in CTE of ferrite in comparison with pure iron are within 3.6% above 450 °C (16.4 × 10−6 K−1 in ferrite-pearlite
microstructure, 16.2 × 10−6 K−1 in the tempered martensite and
16.1×10−6K−1inthebainite,Fig.5).
Comparing cementite at room temperature in three initial mi-crostructuresandapurecementitepowder[28,29],themeanlattice parametersarequitesimilar(thedifferencesarewithin1%,Table4). Moreover,inthetemperaturerangebetween200and327°C,the vol-umeCTEofcementitereportedin[28]iscloseto42×10−6K−1,which
isingoodagreementwiththeCTEofcementiteobtainedforthethree initialmicrostructuresinthesametemperaturerange:42×10−6K−1for
temperedmartensiteandlowerthan48×10−6K−1forferrite-pearlite
microstructure.Forthetemperaturerangefrom450to600°C,the ob-tainedvolumeCTEofcementite(Table3)isingoodagreementwith literaturedata.
B.Denand,V.A.EsinandM.Dehmasetal.
Fig. 4. Ferrite(black)andaustenite(blue)latticeparametersand cementiteunitcellvolume(green)asfunctionoftemperaturein ini-tialferrite-pearlitemicrostructureonheatingwithdifferentheating rates.(Forinterpretationofthereferencestocolorinthisfigure leg-end,thereaderisreferredtothewebversionofthisarticle.)
Fig. 5. Comparisonofferritemeanlatticeparameterbeforeausteniteformation forthethreeinitialmicrostructuresandforthepureironobtainedonheating witharateof0.25°C/s.InsettablegivesCTEobtainedfromtheexperimental curvesforthetemperaturesbetween450°CandAC1.
Table 4
Meanlatticeparametersofcementiteatroomtemperaturefordifferentinitial microstructuresofa37MnCr4-3steelincomparisonwiththoseforpure cemen-titepowder[28,29]. Microstructure a(Å) b(Å) c(Å) Ferrite-pearlite 5.0858 6.7374 4.5292 Bainite 5.0860 6.7420 4.5301 Temperedmartensite 5.0709 6.7295 4.5484 Cementitepowder[28] 5.0809 6.7530 4.5150 Cementitepowder[29] 5.0901 6.7456 4.5262
4.3. Meanlatticeparametersduringtheferrite+cementite→austenite transformation
Inordertoanalyzethelatticeparameterevolutionsinthe transfor-mationtemperaturerangewithoutthethermalcontribution,the param-etersΔa𝛼,Δa𝛾andΔV𝜃 weredefinedasfollows:foreachphase,the
con-tributionduetothermalexpansionalonewasextrapolatedfrom temper-atureregionswherethisphenomenonwassoleactiveorpredominant, thedifferencewas thencalculated betweenactual measurementand thermalcontributionalone.ThisisschematicallyillustratedinFig.6.
ThiswasdoneassumingaconstantlinearCTEforferriteandconstant volumeCTEforcementitegiveninTable3.
Foraustenite,thevariationsoflatticeparameterwerecalculated tak-ingausteniteinthesingleaustenitedomainasareference.Thisisalso illustratedin Fig.6,wheretheextrapolatedchangesin austenite pa-rametersareshownasatangentlinetothemeasurementsforthehigh temperature,austenitedomain.
The resulting variationsof Δa𝛾, Δa𝛼 andΔV𝜃 areplotted versus austeniteweightfractioninFig.7(a)forferrite-pearlitemicrostructure andinFig.7(b)forallthreeinitialmicrostructures(Δa𝛾andΔa𝛼only).
Δa𝛼slightlydecreasesatthebeginningoftheausteniteformation andremainsnearlyconstantandequalto−1.5×10−4Å between20
and85wt.%ofaustenite.Adropto-1×10−3Å isobservedbetween85
and100wt.%ofaustenite,whatevertheinitialmicrostructure. TheΔa𝛾 variationsareoppositeinsigntothoseofferrite,andten timeslarger.Δa𝛾presentsthehighestvalueatthebeginningofthe trans-formation(0.01Å)andthendecreasesasausteniteamountincreasesto reach 0Å oncethetransformationiscompleted whatevertheinitial microstructure. Thedecrease is largerat thebeginningof the trans-formation.ΔV𝜃 decreases continuouslywithtransformationprogress. Themaximalvalueisnear−0.28Å3correspondingtoarelativevolume
changeof5.210−3.
Thedecreaseinthemeanlatticeparameterofferriteandcementite duringthetransformation,whichissmallbutsignificantcanbe associ-atedwiththedevelopmentofcompressivestresses[30]orwithachange initschemicalcomposition.
Sincetheaustenitehasalowyieldstressinthetemperaturerange wherethetransformationoccurs,thechangesinitslatticeparameters shouldbemainlyassociatedwithchemicalcompositionvariation.
4.4. Austenitechemicalcompositionduringaustenitization
Consideringonlythesoluteelementsinthestudiedsteel,weusedthe relationproposedbyDysonandHolmes[31],asdonein[32–34],forthe latticeparameteroftheausteniteasafunctionofchemicalcomposition (inwt.%)atroomtemperature:
𝑎𝛾 =3.5847+0.0330 × [C]+0.00095 × [Mn]−0.0002 × [Ni]
+ 0.0006 × [Cr]+0.0015 × [Cu] (1)
where3.5847Å correspondstotheaustenitelatticeparameterinthe pureironatroomtemperature.
UsingthecompositionprovidedinTable1,theaustenitelattice pa-rametercanbecalculatedto3.59789Å.Thisis0.01319Å greaterthan forpureiron,withacontributionof0.01175 ˚Aduetocarbonalone,and of0.00144 ˚Aduetothesubstitutionalelements.Giventhatthecarbon
Fig. 6. Ferriteandaustenitelatticeparametersandcementiteunit cellvolumeobtainedforferrite-pearliteinitialmicrostructureon heatingof0.25°C/s.Δa𝛼,Δa𝛾andΔV𝜃areschematizedbyarrows.
Fig. 7. Variationsofmeanlatticeparametersofferriteandaustenitewithoutthermalcontribution(Δa 𝜶andΔa 𝜸,respectively)andunitcellvolumeofcementite (ΔV 𝜽)asafunctionofausteniteweightfractiononheatingof0.25°C/sfor(a)ferrite-pearliteand(b)threeinitialmicrostructures.
influenceistherefore10timeslargerthanthatofthesubstitutional el-ements,thevariationsofΔa𝛾,maybeassumedtobemainlyrelatedto changesincarbonconcentrationinaustenite(Δwc𝛾).Thisisexplicited
inEq.(2):
Δ𝑎𝛾=𝐴× Δ𝑤𝑐𝛾 (2)
with𝐴=0.033∀∕wt.%[31].
UsingEq.(2)andconsideringthattheaustenite hasthenominal carboncontentofthesteel,wc0𝛾(Table1),oncetheaustenitizationis
completed,themeancarboncontentintheaustenite(wc𝛾)canbe esti-matedatanymomentofthetransformationusingthevariationoflattice parameteraftersubtractionofthermalcontributionΔa𝛾:
𝑤𝛾 𝑐=
Δ𝑎𝛾
𝐴 +𝑤𝑐0𝛾 (3)
TheresultofsuchestimationisgiveninFig.8forferrite-pearlite andtemperedmartensiteinitialmicrostructuresandfordifferent heat-ingrates.
Whatevertheconsideredinitialmicrostructureandheatingrate,a continuousdecreaseinthemeancarboncontentinausteniteisobserved untiltheendoftheaustenitization,whenthecarboncontentstabilizes andremainsconstantduringfurtherheating.Thecarboncontentinthe
first 3wt.% ofaustenite(“initial” austenitemeancarbon content)is equalto0.59wt.%fortheinitialferrite-pearlitemicrostructureandthe lowestheatingrateof0.25°C/s.Anincreaseintheheatingrateleads toanincreaseinAC1temperatureandtoadecreasein“initial” mean carboncontentinfreshaustenite(0.54wt.%for10°C/sand0.44wt.% for100°C/s).Asimilarbehaviorisobservedfortheinitial microstruc-ture of temperedmartensite(Fig.8(b))with lessdifferencebetween the“initial” meancarboncontentinausteniteforthedifferentheating rates.
Marking theend ofcementitedissolution, differentstagescan be outlined(Fig.8):afirstonewithasharpdecreaseincarboncontentin austenitebetweenthebeginningofthetransformationandthecomplete dissolutionofcementiteandasecondonewithasmootherdecrease cor-respondingtotheremainingferritedissolution.Oncetheaustenitization iscompleted,thecarboncontentinausteniteremainsconstantandequal tothemeancarboncontentofthestudiedsteel.
Whentheheatingrateincreases,thecementitedissolutionfinishes athighertemperaturesandthecorrespondingmeancarboncontentin austenitedecreasessinceahigherferriteamounttransformsinaustenite beforecompletecementitedissolution[15].
The mean carbon contentevolution in austenite during thetwo stagesoftheaustenitizationintheferrite-pearliteinitialmicrostructure
B.Denand,V.A.EsinandM.Dehmasetal.
Fig. 8. Meancarboncontentinausteniteandaustenitefractionversustemperatureduringaustenitizationfordifferentheatingratesandtwoinitialmicrostructures: (a) ferrite-pearliteand(b)temperedmartensite.
Fig. 9. Meancarboncontentinausteniteandaustenitefractiononheating dur-ingaustenitizationofinitialbainiticmicrostructurefordifferentheatingrates.
heatedat0.25°C/scanbefurtheranalyzed.FromresultsshowninFig.8, thecarboncontentinausteniteattheendofpearlite(i.e.,cementite) dis-solutionisabout0.45wt.%correspondingtothemeancarboncontent intheinitialpearlite.Indeed,thepearlitefractionestimatedbyimage analysisfromimagesacquiredonScanningElectronMicroscope(SEM, Fig.1(a))wasfoundtobe80%.Consideringthatthereisnocarbonin ferrite,themeancarboncontentinpearlitecanberoughlyestimatedas
0.356
0.8 =0.445wt.%,whichagreeswellwith0.45wt.%estimatedfromin situexperimentasdiscussedabove.
FromFig.8,weconcludethatforthelowestheatingrateof0.25°C/s, thefirstformedaustenitehasahighercarboncontent(0.59wt.%)than themeancarboncontentin theinitialpearlite (0.44wt.%).As tem-peratureandaustenitefractionincrease,themeancarboncontentin austenitedecreasesuntilreachingthemeancarboncontentofthe ini-tialpearliteattheendofthefirststageofthetransformation.During thesecondstageofthetransformation,thedissolutionoftheremaining 20%offreeferritewithnegligiblecarboncontentoccursandthemean carboncontentinaustenitedecreasesmoresmoothly.
Inthecase ofbainiticmicrostructure, adecreasein meancarbon contentinausteniteisalsoobservedduringthetransformation. How-ever,theinitialcarboncontentinausteniteincreaseswiththeheating rate(Fig.9).Such aresult,differentfromthoseobtainedforthetwo
otherinitialmicrostructuresshouldbeexplainedusingthe microstruc-turaldifferencesindifferentinitialstatesofthestudiedsteel.Indeed, asmallamountofretainedaustenitewasfoundintheinitialbainitic microstructureunliketheferrite-pearliteandthetemperedmartensite microstrutures.Fortheheatingrateof0.25°C/s,theretained austen-itecompletelytransformsintoferriteandcementitebetween240and 410°C.Fortheheatingratesof10°C/sand100°C/s,theretained austen-ite(initialfractionof3wt.%)isnotcompletelytransformedwhen reach-ingAC1temperatureandthetransformedaustenitefractiondecreases
with increasein heatingrate(about0.7 wt.%at745 °Cfor 10 °C/s and2wt.% for100 °C/s).Keepingthe assumptionthat theinternal stressesarerelaxedinausteniteatthosetemperatures,thehighercarbon contentintheaustenitewhenreachingAC1temperatureforincreased heatingratemayberelatedtothecarbonenrichmentoftheretained austeniteduringthebainitictransformation[35].Apartial transforma-tionoftheretainedausteniteinferriteandcementite(heatingrateof 10°C/s)couldthusleadtoaglobalincreaseinthecarboncontentin austeniteatthefirstmomentofaustenitization(for3wt.%ofaustenite) (Fig.9).OncetheAC1temperatureisreachedandaustenitefraction
in-creases,themeancarboncontentinaustenitestartstodecreasedueto ferrite+cementite→austenitetransformationasfortheother microstruc-tures.
Inadditiontothemeancarboncontentinaustenite,itschemical ho-mogeneitycanbeestimatedusingtheFWHM(full-widthheightmiddle) ofdiffractionpeaksrecordedduringinsituexperiments.Accordingto Caglioti’sequation,FWHMvarieswiththediffractionangle𝜃[36]:
FWHM=
√(
𝑈× tan2(𝜃)+𝑉× tan(𝜃)+𝑊) (5) whereU,V,Warethehalf-widthparametersthatcanbeobtainedby Rietveldrefinement.
First,thediffractiondiagramswiththe(111)𝛾and(200)𝛾peaksare giveninFig.10forthreeaustenitefractionsandferrite-pearliteinitial microstructureheatedat0.25°C/s.TheyillustratethelargerFWHMat thebeginningofthetransformation(6wt.%ofaustenite).
TheFWHMevolutionfor(111)𝛾and(200)𝛾peakscalculatedusing theCaglioti’sEq.(5)areplottedversus temperatureinFig.11.2 For
easeofcomparison,themeancarboncontentinaustenitepreviously discussedisalsoreported.AstrongcontinuousdecreaseintheFWHMof
2 AsthesameevolutionsofFWHMfordifferentmicrostructureswithincrease inheatingrateswereobserved,Fig.11reportsthedataforthreemicrostructures andthreedifferentheatingrates.
Fig. 10. Austenitediffractionpeaks(111)and(200)correspondingto differ-entstagesofausteniteformationonheatingwiththeheatingrateof0.25°C/s ininitialferrite-pearlitemicrostructure:6wt.%(beginning),66wt.%(endof cementitedissolution)andfullyaustenitic(endoftheaustenitization). (111)𝛾and(200)𝛾peaksisobservedduringthefirststageofthe austen-iteformationfollowedbyaplateauduringthesecondstage(remaining freeferritedissolution)andlateronceausteniteformationiscompleted. Anenlargementindiffractionpeaksmaybeduetoseveralfactors: smallsize of diffractingdomains, heterogeneities(chemical,internal
stresses,localtemperature).ThedecreaseinFWHMcanbemainly as-sociatedwithahomogenizationofcarboncompositionoftheaustenite becausestressandthermalgradientduringausteniteformationas dis-cussedearliercanbeconsiderednegligible.Indeed,gradientsincarbon contentarepresentduringthetransformation.Thechemical homoge-nizationbeingcontrolledbydiffusion,isacceleratedwithtemperature. TheFWHMofaustenitediffractionpeaksisthusmaximalatthe begin-ningofthetransformationduetoamaximumchemicalheterogeneity. Moreover,itisworthnotingthatthemaximumFWHMincreasesasthe heatingratesincreasesuggestingincreaseinchemicalheterogeneities inaustenite.
5. Discussion
Sinceanydataforthechemicalcompositionofdifferentphasesin differentinitialmicrostructureswerenotavailable,severalassumptions arerequiredforfurtherdiscussion.Threeinitialmicrostructureswere obtainedatdifferenttemperaturesandfordifferentdurations:625°C - 1hforferrite-pearlite,425°C-30minforbainiteand500°C-1h fortemperedmartensite.Thesethreetemperaturesandcorresponding durationsseemtobedisadvantageousforasignificantdiffusiondistance ofthesubstitutionalelements(Si,Mn,Ni,Cr,MoandCu).Indeed,the estimationofthebulkdiffusionlengthsinaustenitefortheseelementsat thehighesttemperatureof625°Cfor1hannealing,indicatethatitdoes notexceed10nmforthefastdiffusingelementslikeCrandMn[37]. However,thecementiteinpearlitecanbesignificantlyenrichedinMn eventhoughthepearliteformationtakesplaceatlowtemperaturesdue toacceleratedMndiffusionalongtheinterfaces[38,39].Nevertheless,
Fig. 11. FWHMof(111)𝛾and(200)𝛾diffractionpeaksofaustenitecomparedtothemeancarboncontentevolutionduringausteniteformationfordifferentinitial microstructuresandheatingrates:(a)ferrite-pearliteat0.25°C/s,(b)bainiteat10°C/s,(c)temperedmartensiteat100°C/s.
B.Denand,V.A.EsinandM.Dehmasetal.
Table 5
Austenitestarttemperature(AC1)andmeancarboncontentinausteniteatthebeginningofaustenitization(C0𝛾)(3wt.%offormedaustenite)fordifferentheating
ratesandinitialmicrostructures.
Heatingrate(°C/s) Ferrite-pearlite Temperedmartensite Bainite
AC1(°C) C0𝛾(wt.%) AC1(°C) C0𝛾(wt.%) AC1(°C) C0𝛾(wt.%)
0.25 740 0.594 736 0.593 736 0.585
10 761 0.543 742 0.586 – –
100 781 0.442 753 0.554 – –
Fig. 12. Isoplethphasediagramforthe37MnCr4-3steelforfixedcontentof substitutionalelementsandvaryingcarboncontent(attheexpenseofiron) ob-tainedusingThermo-CalcsoftwareandTCFE9database.Mncontentwastaken 1.285wt.%(blacklines)andcorrespondingto5,10and20wt.%(dashed col-oredlines)ofMnincementiteinequilibriumwithaustenitetotakeintoaccount eventualMnenrichmentincementiteduringpearliteformation.Initialcarbon contentinausteniteobtainedexperimentally(points)iscomparedwiththemean carboncontentinaustenite,whichisinthermodynamicequilibriumwith fer-riteandcementitehavingthesamecontentofsubstitutionalelements(dotted greenline).(Forinterpretationofthereferencestocolorinthisfigurelegend, thereaderisreferredtothewebversionofthisarticle.)
diffusionofsubstitutionalelementsduringtheformationoftempered martensiteandbainiteshouldbesufficientlylimitedtobeneglected.
Therefore,onecan expectthesame contentofsubstitutional ele-ments(thesameu-fraction)inferriteinbainiteandtempered marten-sitemicrostructureswhilesomeMnpartitioningcouldtakeplaceduring thepearliteformationleadingtocementiteenrichedbyMn.Duringthe austenitization,Mn partitioningcanoccuraswell whichdepends on initialMncontentinferriteandcementite[40,41].
Wenowcananalyzetheformationoffreshausteniteusingan iso-plethphasediagramobtainedforthefixedcontentofthesubstitutional elements(accordingtoTable1),exceptthatofMn,andvaryingcarbon content(attheexpenseofiron)usingThermo-CalcsoftwareandTCFE9 database(Fig.12).Inordertotakeintoaccountpossiblecementite en-richmentbyMnduringpearliteformationorduringslowheatingrate ofthethreeinitial microstructures,Mncontentincementitein ther-modynamicequilibriumwithaustenitewasbeingvariedwhenplotting isoplethdiagram.However,onecanobservethatdifferentMncontent incementite(from5to20wt.%)inequilibriumwithaustenitedoes notchangesignificantlyaustenite/cementiteequilibriumascompared toglobalcontentofMnof1.285wt.%(Fig.12).Therefore,the discus-sioncanbelimitedtothenominalMncontentinthestudiedsteelof 1.285wt.%.
Theisoplethphasediagramfor1.285wt.%ofMn(blacklines)gives carboncontentintheausteniteinequilibriumwithcementitec𝛾/𝜃and
ferritec𝛾/𝛼havingthesamecontentofsubstitutionalelementsasthatin
austenite.
Plottingtheinitialmeancarboncontentinausteniteobtainedfrom theinsituexperiments(pointsinFig.12),weobservethatforthe heat-ingrateof0.25°C/s(thelowestaustenitestarttemperature),the austen-itemeancarboncontent,atthestartofaustenitization,isclosetothe eutectoidcomposition,butnearertothecompositionoftheausteniteat equilibriumwithcementite.Thecarboncontentoffreshausteniteclose tothatofeutectoidcompositionwerereportedin[4,40,42]and sug-gestedrecentlyin[15]whereausteniteformationisstartingcontrolled bycarbondiffusion[40,41,43–47].
Fordifferentheatingratesandferrite-pearliteandtempered marten-sitemicrostructures,adecreaseofthemeaninitial carboncontentin austeniteisobservedwhenheatingrate(andthus theaustenitization starttemperature(AC1))increases(Table5).
Whenwereportallexperimentalvaluesofinitialcarboncontentin austeniteontheisoplethphasediagram,weobservethatincreasingthe heatingrate,theinitialmeancarboncontentinaustenitevaries accord-ingtotheaveragevalue(c𝛾/𝛼+c𝛾/𝜃)/2(Fig.12).Sucharesultsuggestsa
lineargradientforcarboncontentinthefirstausteniteformedbetween ferriteandcementite[48].
Inthecaseoftheferrite-pearliteinitialmicrostructureandtherate of100°C/s,adeviationfromtheaveragevalue(c𝛾/𝛼+c𝛾/𝜃)/2is ob-served.Eventual partitioningof Mnduringaustenitization andwhen forminginitialferrite-pearlitemicrostructureshouldbecarefully exam-inedforfastheatingrate.Theassumptionofnon-linearcarbonprofilein austenitecanbesupposed.Experimentally,itrequiresadditional anal-ysisofchemicalcompositionofphasesininitialmicrostructuresbefore austenitization.
6. Conclusion
Theinfluenceofheatingrateandinitialmicrostructureonthemean latticeparametersofferrite,cementiteand,especially,thatofaustenite duringaustenitizationwasinvestigatedbyinsituHE-XRDina 0.36C-1.3Mn-0.7Cr-0.07Mowt.%steel.Themainresultsaresummarized be-low:
(1) Ferriteandcementiteareundercompressionattheendoftheir transformationintoaustenite;
(2) Duringtheaustenitization,themeanlatticeparameterof austen-itedecreases;thisdecreaseismainlyassociatedtoachangein themeancarboncontent;
(3) Assumingthattheelasticstrainsinaustenitearenegligible,the variationsinmeancarboncontentinaustenitearecalculated us-ingmeanaustenitelatticeparameterforeachtransformation con-dition.Thefirstformedaustenitehasthehighestmeancarbon content;itdecreasesrapidlydue tothesimultaneous transfor-mationofferriteandcementiteintoaustenite.Oncecementite isdissolved,duringtheferritetransformation,themeancarbon contentinaustenitedecreasesmoreslowly;
(4) Theinitial meancarbon contentin austeniteat thebeginning oftheausteniteformationisdependent ontheheatingrate:it decreasesasheatingrateincreases(asclearlyshownfor ferrite-pearliteandtemperedmartensiteinitialmicrostructures).Forthe lowestheatingrate,thecarboncontentinthefirst3wt.%formed austeniteisnearthecalculatedeutectoidcompositionobtained byThermo-CalcandTCFE9database;
(5) Valuesofinitialcarboncontentinthefirstausteniteformedarein goodagreementwiththermodynamiccalculationswithor with-outpartitioningofMnininitialcementite.
DeclarationofCompetingInterest
Theauthorsdeclarethattheyhavenoknowncompetingfinancial interestsorpersonalrelationshipsthatcouldhaveappearedtoinfluence theworkreportedinthispaper.
Acknowledgements
Authors gratefully acknowledge the Deutsches Elektronen-Synchrotron (DESY, Hamburg, Germany) and staff of the P07 line atPETRAIII, especially,Andreas Starkfor theassistancewithX-ray diffraction experiments. Financial support of the National Research Agency (ANR) (research grant No. ANR-2010-RMNP-011-06) is gratefullyacknowledged.
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