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熱烈法玻璃激光切割技術(shù)綜述Contents1234IntroductionTypicalExperiments&ResultsComparison&ProspectReferencesIntroductionThe
traditionalmethodsofglasscuttingarebasedonscoringandsnappinginwhichadiamondbladetoolisusedforscribing,whichweakenstheglasssurfaceandthenbreakingisdonebyapplyingthemechanicalforce.Althoughthemethodisrelativelysimple,itresultsintheweakeningofglassedgesbyupto60%duetotheformationofmicrocracksandgenerationofresidualstresses.Toreducethesedefects,glasscanbegrounded,polished,andheattreatedbutthesetechniquescanonlyrecoveronlyupto30%oftheglassstrength.IntroductionDifferent
techniquesofcuttingglassusinglaserexistssuchaslaserscribeandbreak,lasermeltingandevaporation,andthecontrolledfracturetechniquefromwhichsomearebeingusedinindustriesandsomearestillintheirdevelopmentalstages.Laser
scribeandbreakisatwostageprocessandisquitesimilartotraditionalmechanicalscribeandbreakmethod.Inthefirststage,partiallypenetratingholesordeepventsatdepthsofonethirdtoone-halfofthematerialthicknessareproducedusingalaser.Inthesecondstage,breakingbyapplyingamechanicalforcetakesplacenormallywiththehelpofvacuumchucksorbycrackrollers.Severalstudieshavebeendonetoimprovethismethodandthecuttingquality.However,thescribingandbreakingprocessincursdamagetothecutedgeandcausesdamagetotheglasssurface.Therefore,finishingprocessesarerequired,whichaddextracosttothemanufacturer.IntroductionIn
lasermeltingandevaporationmethod,cuttingisdoneabove
glasstransitiontemperatureTg,whichresultsinpoorsurfacefinishandheataffectedzones.Duetomeltingandvaporizationof
theglassmaterialduringcutting,microcracksandburrsaregeneratedalongthecuttingprofileandtherequirementofgrinding
andpolishingattheendoftheprocessbecomesinevitable.Ascomparedwithlaserscribeandbreakandlasermeltingandevaporationmethod,thecontrolledfracturetechniqueisasinglestageprocessinwhichcuttingisperformedbelowtheglasstransitiontemperatureTg,whichresultsinsmoothedgesandhencerequiresnofurthercleaningorgrinding.Unliketheconventionalcuttingtechnique,itisacleanprocesswithoutchipsandcoolantanditispossibletofixtheworkpieceonatablebyasimplemethodbecausenoexternalforcesactuponit.IntroductionInthecontrolledfracturetechnique,thecracksareinitiatedduetoabsorbedphotonsheatingupthematerial.Thestressesnearthelaserspotarecompressiveduetohightemperature.Afterthepassageofthelaserbeam,thesecompressivestressesrelaxandinducelocalresidualtensilestresses.IfthesestressesexceedthefailurestressσfgivenbythecriticalstrainenergyreleaserateσGcforglass,crackpropagates.TypicalExperiments&ResultsIn2008KojiYamamotoet.al.conductathree-dementationalthermalanalysisonlaserscribingofglass.TheyshapeaCO2laserbeamanelliptical(橢圓)profilewhichhasanominalpowerof250Wandawavelengthof10.6μmtoirradiateonthesurfaceoftheglassplate.ExperimentsTypicalExperiments&ResultsResultsTheDcmax
takesitsmaximumat
d=14–16mm.Above18mm,Dcmaxtends
to
decreaseproportionallytod.Thiscanbeinterpretedaswith
increasingd,theheatdiffusionreducestheglasssurfacetemperatureimmediatelybeforethecooling,sothatthedifference
decreasesbetweenthesurfacetemperatureand
theinside
temperatureinthecoolingarea.ParametersLaserPowercoolingmediumTherearemanyparameterswillinfluencethelasercuttingwithcontroledfracture.Suchasthepoweroflaserandthethermalexpansioncoefficient,heattransfercoefficientandsoon.ScanningVelociycoolingpointdistancethermalexpansioncoefficientTypicalExperiments&ResultsThenKojiYamamotoet.al.choosetostudytheinfluenceofglasssubstratethicknessandthermalexpansioncoefficientinlaserscribingofglass.GlassSubstrateThicknessThermalExpansinCoefficientTypicalExperiments&ResultsSalmanNisaret.al.studiedtheinfluenceoflaserbeamgeometryindiodelaserchip-freecuttiingofglass.TypicalExperiments&ResultsResultsComparison&ProspectStressTypicalExperiments&ResultsAverageRoughnessTypicalExperiments&ResultsTemperatureComparison&ProspectInthesecondpart,manyexperimentsareconductedbylotsofresearchers.Wecanconcludetheirresearchesthatlasercuttingqualitywillmainlydependonthemaximumtemperatureinthesurfaceofglassandthemaximumtensilestressinthecoolingarea.Sowhichparameterwillaffectthetwofactors.Thethicknessofglasswillaffectthemaximumtensilestressinthecoolingarea,andhollowswillforminthebacksideofthelowerthicknesssubstrate.Thetensilestressgeneratedinthecoolingareadecreasesasthethermalexpansioncoefficientdecreases.Itisconcludedthatbecauseoflowermagnitudesoftensilestressesσxx,thetri-fbeamgivesminimumcutpathdeviationattheleadingedgeandtri-randcircularbeamsgiveminimumcutdeviationatthetrailingedgeoftheglasssheet.Comparison&ProspectTheresultspresentedinthesepapersareimportantfortheoptimizationofthelasercuttingprocessofglass.However,moreworkisneededtostudytheoptimumbeamshapealongwithotherlaserparametersi.e.,laserpower,cuttingspeed,andbeamspotsizetofurtherminimizecutpathdeviationattheleadingandtrailingedgesoftheglasssheet.Sointhenextfuture,wemaytryevenmorelaserparameterstofindheoptimumbeam.Butitmustbeinareasonableway.Suchas"Orthogonalexperimentaldesign".Wecanchoosethemainfactorstodoaorthogonalexperimentaldesign,thencompletetheexperimentandcomparetheresultsofittillwefindtheoptimumparametersandcuttingpath.Refe
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