凝胶的机械性能醇凝胶气凝胶眼镜.docx
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凝胶的机械性能醇凝胶气凝胶眼镜
MechanicalPropertiesofGels:
FromAlcogelandAerogelstoGlasses
INTRODUCTION
Themostfascinatingfeaturesofgels(lowsoundvelocity,highspecificsurfacearea,lowthermalandelectricconductivity…)aregenerallyduetotheirverylargeporosity,whichcanbeashighas99%.However,thecounterpartofthishugeporosityispoormechanicalpropertiesandtheconsequenceisthatgelstendtocrackduringdrying.So,oneofthemostdifficultproblemsinsol–gelscienceistomakelargebodiesofdriedgels(xerogelsoraerogels).
Thedryingstressesareattributedtocapillaryphenomenaanddifferentialstrainwhichresultfromapressuregradientintheporeliquid(Brinker,1990).Differentwayshavebeenstudiedtosolvethisproblemandforexamplesupercriticaldrying(SD)allowsonetoavoidthecapillarystressesandmonolithicaerogelcanbeobtained(Kistler,1932).
Thepotentialitiesofthismaterial(Cerenkovdetector,acousticorthermalinsulator,hostmatrixforcatalysts)areincreasedifconsiderednotonlyasanendproduct,butasaprecursor.Byasetofsinteringtreatments,thesilicaaerogelscanbeeasilytransformedintopuresilicaglass(Woignier,1990)andappropriateheattreatmentsleadtoPartiallyDenseAerogel(PDA)whichcanbeusedasahostmatrixforthesynthesisofdopedglassesorcomposites.
Theknowledgeofthemechanicalpropertiesofgelsandaerogelsisofinterestfortechnologicalapplications,butalsofortheoreticalresearch.Gelsareidealmaterials,inthesensethattheevolutionofphysicalpropertiesinrelationwiththestructurecanbeexperimentallystudiedoverthewholerangeofporosity,from0to99%.
Themechanicalbehaviorofgels,xerogelsandaerogels,isgenerallydescribedintermsofbrittleandelasticmaterials,likeglassorceramics(West,1988;Zarzycki,1988;Woignier,1988a).Duringmechanicaltestingevenforveryporousmaterial(99%),thestress–straincurveshowsaperfectelasticbehaviorandtheconchoidalfracturemorphologyindicatesthatthematerialisbrittle,likeaconventionalglass.Themaindifference,comparedtosilicaglass,istheorderofmagnitudeoftheelasticandmechanicalmoduliwhichare104timeslower.However,ifthisanalogyispertinentwhengelsareunderatensionstress(bendingtest),theyexhibitamorecomplicatedresponsewhenthestructureiscompressed(compressiontest).Thenetworkislinearlyelasticundersmallstrains,thenexhibitsyield,followedbydensificationandplastichardening(Pirard,1995;Scherer,1995;Duffours,1995).Asaconsequenceoftheplasticshrinkage,itispossibletoeliminatetheporesandstiffenthegelatroomtemperature.Wewillseethattheseoppositebehaviors(elasticandplastic)aresurprisinglyrelatedtothesametwokindsofgelfeatures:
thesilanolcontentandtheporesizedistribution.Differentkindsofgelstructure(fractalornotfractal)havebeensynthesized,throughacontrolofthedifferentstepsoftransformation,suchassinteringandplasticcompactionandwerestudiedasafunctionoftheirstructure.Theinfluenceofthesinteringprocess,comparedtotheplastictransformation,ontheelasticpropertiesandmechanicalbehaviorareexplainedbytheassociatedstructuralchanges.Therelationshipsbetweenstructuralandmechanicalpropertieswillbediscussedintermsofthecellularmodel,percolationtheory,fractalstructureandtheblobsandlinksmodel.
EXPERIMENTALPROCEDURE
Differentfamiliesofgelshavebeenelaboratedforthesestudies.Themainaresilicaalcogelsandaerogels.Thealcogelsarepreparedbyhydrolysisandpolycondensationreactionsoftetramethoxysilane(TMOS).TheTMOSisdissolvedinvariousamountsofethanol,therebyadjustingtheoxidecontentofthesol(andthefinalbulkdensityofthematerial).Thesolutionsarehydrolyzedunderneutral,basic(NH4OH,5×10–2N)oracidic(HNO3,10–4N)conditions.Thealcogelsaretransformedintoaerogelsbysupercriticalevacuationofthesolvent.Forseveralsamples,thesupercriticalheattreatmentisnotfollowedbytheevacuationofthesuperfluid,sothesolventinvadesthegelduringcooling.Theinterestofthisprocedureistopreparematerialsfullofsolventforwhichthesolidnetworkhasundergonethesameheattreatmentasforclassicalaerogels.Thesesamplesarecalled“re-wettedaerogels”.ThesamplesarelabeledN,BorA(withrespecttothecatalyst),followedbytheTMOSweightpercent.
Thedensificationoftheaerogelsisobtainedbyheattreatmentatatemperatureof1050°Cand,asafunctionofthesinteringtime,thebulkdensityincreases.ThesamplesarelabeledPDAxx(PartiallyDenseAerogel)wherexxisthebulkdensityexpresseding/cm3.ThePCAxxsamples(PartiallyCompressedAerogel)correspondtogelswhosedensityhasbeenincreasedbyroomtemperaturecompression.
Theelasticmoduliandthemodulusofruptureofthesamplesweremeasuredbythe3-pointsbendingtechnique,usinganInstrontestingmachinewitha20Nloadcellandbysoundvelocity.ThefracturetoughnesswasmeasuredusingtheSingleEdgeNotchedBeam(SENB)methodinthethreepointbending.Generally,thebeambendingdataallowcalculationoftheYoung’smodulus;E.Thatistrueforaerogels,but,inthecaseofthealcogelsamples,thebeambendingtestyieldstheshearmodulus.Duetothelowpermeabilityofthealcogels,thefluidforcesthenetworktobehaveasifitwereincompressible.Thenthevolumeofthesampleisunchangedbythedeformationandthefluidexertsatransversestressonthegelnetwork,providingameasurementoftheshearmodulusG(Scherer,1988).Inordertocomparetheelasticpropertiesoftheaerogelsandthealcogels,themeasurementshavebeenmadeonalcogelsandre-wettedaerogels.
Theirstructurewillbecharacterizedbysmallanglescatteringtechniques(SANSandSAXS).Scatteringvectorsq,rangingfrom0.0018to0.3Å–1,wereexploredtoallowadeterminationofthedensity–densitycorrelationfunctioninthelengthscalefrom3to500Å.
MECHANICALBEHAVIOROFALCOGELSANDAEROGELSElasticModuliandMechanicalRupture
Whateverthegoaloftheaerogelsynthesis,itisimportanttoknowhowthesupercriticaldrying(SD)canmodifythephysicalandchemicalfeaturesoftheparentalcogel.Theobjectofthispartistocharacterizetheevolutionofthemechanicalproperties.Wewillstudytheinfluenceofsynthesisparameterssuchastheconcentrationofgelifyingprecursors,pHofthehydrolysissolutionandaging,onthephysico-chemicaltransformationsobservedduringthesupercriticalfluidextraction.Intheliterature,mechanicaltestinghasbeenmadeeitheronalcogels(West,1988;Zarzycki,1988;Scherer,1988),oronaerogels(Calemczuk,1987;Dumas,1990;Woignier,1988b;Gross,1992)andcomparisonofthetwosetsofdatasuggeststhatsupercriticaldryingenhancesthemechanicalfeaturesofthesamples.Theapplicationoflinearelasticfracturemechanicstowetgelsisquestionable,becauseitisnecessarytojustifythatthematerialhasanelasticbehaviorandcanbetreatedasacontinuum.Scherer(1992)hasdiscussedthisproblemandhasshownthatitseemsreasonabletoapplyfracturemechanics,becausetheelasticregionnearthetipofthecrackismuchlargerthantheplasticdeformationatthecracktip.Aspreviouslymentioned,thebeambendingtestyieldsdifferentelasticmoduliforalcogels(G)andforaerogels(E).IfwewanttofollowtheinfluenceofSDonthemechanicalfeatures,theshearmodulushasbeenmeasuredonalcogelsandre-wettedaerogels.GcanalsobecalculatedfromEandthePoisson’sratiov.TheshearmodulusisrelatedtoEbyE=2(1+v)G.ThePoisson’sratio,measuredbyBrillouinscatteringandsoundvelocitypropagation,iscloseto0.2overthewholerangeofaerogeldensityandfordifferentcatalysts.InfactGcalculatedfromEandvandGmeasuredonre-wettedaerogels,givesimilarresults(Woignier,1992).
Figure14-1showstheinfluenceofSDonthemechanicalproperties,Gandthemechanicalstrengthσofaneutralsetofsamples.ItisclearthatGandσincreasebyafactorof10–20.TheeffectofconcentrationisalsoshownandobviouslythemechanicalpropertiesimprovewiththeTMOSconcentration,overalmost2ordersofmagnitude.However,duringSD,ashrinkageisobservedandthechangeofthemechanicalpropertiescouldbeattributedtothisshrinkage,whichincreasestheloadbearingfractionofsolid.InFigure14-2,theshearmodulusofthedifferentsetsofsamples(neutral,basicandacid)havebeenplottedasafunctionofthefractionofsolids.Gvaluesofre-wettedaerogelsarestillhigherbyafactor4–5.Thisfigureshowsalsothat,iftheacidicandneutralsampleshavenearlythesamemechanicalproperties,forthebasicset,thevaluesofGarelower.
Figure14-1.EvolutionoftheelasticandmechanicalpropertiesGandσasafunctionoftheTMOScontentfortheneutralsetsofalcogelsandre-wettedgels
Figure14-2.EvolutionofGasafunctionofthebulkdensityforneutral,acidandbasicsetsofalcogelsandre-wettedgels.
ToexplainthestrengtheningofthematerialsduringSD,wecaninvoketwokindsofprocessesoccurringintheautoclave.Thefirstmustberelatedtotheformationofsiloxanebondsbetween“danglingbonds”inthealcogel.Thesebondscontributetothemass,butnottotheconnectivityofthenetwork.Whentwobranchescomeintocontact,condensationreactionsofsilanolgroupstakeplace,increasingtheconnectivity.Thisprocesswouldincreasethestiffnessandthestrength,butwouldalsoimposestressesonthealcogelnetworkwhichcouldexplaintheshrinkage.Thesecondmechanismofstrengtheningisduetothegrowthofthenecksbetweenparticles.Thisgro