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52 LCGC NORTH AMERICA VOLUME 22 NUMBER 1 JANUARY 2004 www.chromatographyonline.com temperature-rising elution fractionation overcomes the limitations of preparative temperature-rising elution fractionation by reducing the column and sample sizes con- siderably and by continuously monitoring the amount of the eluted polymer fractions as a function of column temperature using an on-line detector. For polyethylenes, the major factor that determines melting in a solution is the degree of short-chain branching (3). Each branching point in a chain is rejected from the growing crystal, thereby limiting crystal thickness and hence reducing the melting temperature. Thus, a direct relationship exists between the melting temperature and the degree of branching, which is reflected in analytical temperature-rising elution frac- tionation curves. Moreover, Nagano and Goto (3) and Mirabella (4) have reported that a linear relationship exists between the elution temperature and the degree of short- chain branching (number of branches per 1000 carbon atoms). Therefore, analytical temperature-rising elution fractionation curves do in fact describe the short-chain branching distribution (5). The short-chain branching distribution provides some information about the mech- anism of polymerization and the nature of the catalysts. As an example, when chemists use conventional Ziegler-Natta catalysts for the polymerization of ethylene, a broad The authors describe a system for automated analytical temperature-rising elution fractionation that uses the built-in differential refractometer of a commercial gel-permeation chromatography instrument and a stop-flow method for sample crystallization. They discuss the performance of the system and its ability to fractionate different types of polyethylenes. An Improved Analytical Temperature-Rising Elution Fractionation System for Automated Analysis of Polyethylenes Adrian G. Boborodea*†, Daniel Daoust*, Alain M. Jonas*, and Christian Bailly* * Catholic University of Louvain, Unité de Physique et de Chimie des Hauts Polymères, Bâtiment Boltzmann, Place Croix du Sud, 1, B-1348 Louvain-la-Neuve, Belgium, e-mail boborodea@ poly.ucl.ac.be Polytechnical University of Bucharest, Department of Polymer Physics, 149 Calea Victoriei, Sector 1, Bucharest, Romania Address correspondence to A.G. Boborodea. olymers basically are heteroge- neous materials, and heterogene- ity can be exhibited in various ways such as distribution of chain lengths, differences in chemical composi- tion, stereoregularity, and architecture (tac- ticity or branching). Branching can be char- acterized as either long chain or short chain. Temperature-rising elution fractionation is a technique that allows the analysis of semicrystalline polymers by separating frac- tions according to their crystallizability. Temperature-rising elution fractionation enables analysts to evaluate structure hetero- geneity and to characterize the distribution of short-chain branching. Elution during temperature-rising elution fractionation is governed by the melting of semicrystalline polymers in the presence of a solvent (1). Preparative temperature-rising elution fractionation can be performed to isolate fractions for additional investigations. Dur- ing this process, a large quantity of solvent is required for eluting the sample, and a large amount of non-solvent, usually meth- anol, also is used for precipitating the eluted fractions (2). This technique is quite time- consuming; it typically requires several days to perform a fractionation. The development of analytical temperature- rising elution fractionation has been an improvement upon preparative temperature- rising elution fractionation. Analytical P

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52 LCGC NORTH AMERICAVOLUME 22NUMBER 1JANUARY 2004 www.chromatographyonline.comtemperature-risingelutionfractionationovercomesthelimitationsofpreparativetemperature-risingelutionfractionationbyreducingthecolumnandsamplesizescon-siderablyandbycontinuouslymonitoringthe amount of the eluted polymer fractionsasafunctionofcolumntemperatureusingan on-line detector.Forpolyethylenes,themajorfactorthatdeterminesmeltinginasolutionisthedegreeofshort-chainbranching(3).Eachbranchingpointinachainisrejectedfromthe growing crystal, thereby limiting crystalthicknessandhencereducingthemeltingtemperature.Thus,adirectrelationshipexists between the melting temperature andthe degree of branching, which is reected inanalyticaltemperature-risingelutionfrac-tionationcurves.Moreover,NaganoandGoto(3)andMirabella(4)havereportedthatalinearrelationshipexistsbetweentheelution temperature and the degree of short-chainbranching(numberofbranchesper1000carbonatoms).Therefore,analyticaltemperature-risingelutionfractionationcurvesdoinfactdescribetheshort-chainbranching distribution (5).Theshort-chainbranchingdistributionprovides some information about the mech-anismofpolymerizationandthenatureofthe catalysts. As an example, when chemistsuseconventionalZiegler-Nattacatalystsforthepolymerizationofethylene,abroadThe authors describe a system for automated analytical temperature-risingelution fractionation that uses the built-in differential refractometer of acommercial gel-permeation chromatography instrument and a stop-owmethod for sample crystallization. They discuss the performance of thesystem and its ability to fractionate different types of polyethylenes.An Improved AnalyticalTemperature-Rising ElutionFractionation System forAutomated Analysis ofPolyethylenesAdrian G. Boborodea*,Daniel Daoust*, Alain M. Jonas*, andChristian Bailly** Catholic University of Louvain,Unit de Physique et de Chimiedes Hauts Polymres, BtimentBoltzmann, Place Croix du Sud, 1,B-1348 Louvain-la-Neuve,Belgium, e-mail [email protected] Polytechnical University ofBucharest, Department ofPolymer Physics, 149 CaleaVictoriei, Sector 1, Bucharest,RomaniaAddress correspondence to A.G. Boborodea.olymersbasicallyareheteroge-neousmaterials,andheterogene-itycanbeexhibitedinvariousways such as distribution of chainlengths,differencesinchemicalcomposi-tion,stereoregularity,andarchitecture(tac-ticity or branching). Branching can be char-acterized as either long chain or short chain.Temperature-risingelutionfractionationisatechniquethatallowstheanalysisofsemicrystallinepolymersbyseparatingfrac-tionsaccordingtotheircrystallizability.Temperature-risingelutionfractionationenables analysts to evaluate structure hetero-geneityandtocharacterizethedistributionofshort-chainbranching.Elutionduringtemperature-risingelutionfractionationisgovernedbythemeltingofsemicrystallinepolymers in the presence of a solvent (1).Preparativetemperature-risingelutionfractionationcanbeperformedtoisolatefractionsforadditionalinvestigations.Dur-ing this process, a large quantity of solvent isrequired for eluting the sample, and a largeamountofnon-solvent,usuallymeth-anol, also is used for precipitating the elutedfractions(2).Thistechniqueisquitetime-consuming; it typically requires several daysto perform a fractionation.The development of analytical temperature-risingelutionfractionationhasbeenanimprovementuponpreparativetemperature-risingelutionfractionation.Analytical P54 LCGC NORTH AMERICAVOLUME 22NUMBER 1JANUARY 2004 www.chromatographyonline.combond stretch frequency. IR detection gener-ally is used for analytical temperature-risingelution fractionation because it offers betterbaselinestabilitythandifferentialrefractiveindexdetectionforbothlargevariations of temperature and pressure during the elu-tionprocess(7,1216).However,theIRdetectorhaspoorsensitivityandconse-quently requires the use of large amounts ofpolymerinanalysis.Forthisreason,eitherthe baseline presents a high level of noise (forexample,seereference7sFigure1orrefer-ences 4 and 12s Figure 1) or the peaks con-tainspikes(forexample,seereference8sFigure8orreference15sFigure9).Todecreasethenoiselevel,analystssometimesaveragethechromatogramdatapointsandsmooththecurves(seereference8sFigure11).Thepresenceofahighnoiselevelbecomes even more important when mathe-maticaltransformationsareappliedtoana-lyticaltemperature-risingelutionfractiona-tionchromatogramstoobtainmethylenesequence length distributions for polyethyl-enecopolymers(17)ortopredictdifferen-tialscanningcalorimetrythermograms(4,16,18).Furthermore,IRdetectorsareunavailableoncommercialequipmentandarecomplicatedtoinstall.Forthisreason,theresultsobtainedusingtheanalytical temperature-risingelutionfractionationtechniqueareverydifficulttoreproducefrom one laboratory to another.Inthisarticle,wedescribeanimprovedanalyticaltemperature-risingelutionfrac-tionationsystemthatusesacommercialinstrumentforhigh-temperaturegel-permeation chromatography connected withan oil bath. Our goal was to keep the modi-cation to a minimum by using the existingparts of the chromatograph as much as pos-sible: namely, the automatic injector and thedifferential refractometer, which is more sen-sitivethananIRdetector.Thissystemallowedtheuseofalowerquantityofinjectedpolymer,whichenabledthepossi-bilityofcompletelyautomatingtheprocessby reducing the injected volume of solutionto 200500 L.ExperimentalAnalyticaltemperature-risingelution fractionationapparatus:Theanalyticaltemperature-rising elution fractionation wasperformedusingamodifiedWatersGPC150CVgel-permeationchromatography(GPC)system(WatersCorp.,Milford,Massachusetts) using greater than 99% pure1,2,4-trichlorobenzene(Sigma-AldrichCo.,St. Louis, Missouri) as the solvent. The sol-bimodal distribution of polymer chains withdifferentshort-chainbranchingcontents ispresentinthefinalproductbecauseof themultisitenatureofthesecatalysts(6), ascomparedwithmetallocenecatalysts,which produce a much narrower short-chainbranchingdistribution(7).Short-chainbranchingdistributionandthemolecularmassdistributionhaveamarkedinuenceupon the polymer properties. The shapes ofthesedistributionshaveaprofoundeffectupon the end-use properties of the material,and their determination can generate a morecompleteunderstandingofthebehaviorofpolyethylenes in different applications (8).Several researchers have described systemsfor analyzing a solution of a crystalline or asemicrystalline polymer sample to determineitsshort-chainbranchingdistribution(911).Asageneralmethod,thepolymersamplerstisprecipitatedfromasolutionduring a decreasing temperature gradient toproduce a precipitated polymer sample. Theprecipitatedpolymersamplethenisredis-solved and eluted during an increasing tem-perature gradient to produce successive frac-tionsofthepolymersample,whicharemeasuredtoproduceconcentrationdatafromwhichtheshort-chainbranchingdis-tributioniscalculated.Theconcentrationdetector is a built-in differential refractome-ter (9) or a separate infrared (IR) or nuclearmagneticresonance(NMR)detector(10).In both cases the polymer solution is intro-duced into the fractionation column, whichis placed in an oil bath, using a complex pro-cedurethatrequireshighquantitiesofsol-vent and polymer sample.On the other hand, Yau and Gillespie (11)describeananalyticaltemperature-risingelutionfractionationsystemwithanauto-maticinjectorandanIRdetector.Thisdetectorwastunedto3.48m,theCHventwasstabilizedwith2%ofantioxidantIrganox1010(CibaSpecialtyChemicals,Inc.,Basel,Switzerland).Weplaceda100mm 10 mm stainless steel column packedwith aluminum oxide (70-230 mesh, MerckKGaA,Darmstadt,Germany)inaJulaboF32HPoilbath(JulaboLabortechnikGmbH, Seelbach, Germany).Intherststepoftheanalysisprogram,400 L of solution was injected in the col-umnautomaticallyusingthebuilt-ininjec-toratalowowrateof0.2mL/min.Thislowowratewasusedtoavoidapressure-inducedleakofthepolymersolutionthroughthecolumnafterinjection.Inthesecondstep,theowwasstoppedandthecolumnwascooledintheoilbathat0.5C/min from 135 C to 35 C. In the thirdstep, the polymer was eluted at a ow rate of0.8mL/min,whilethetemperaturewasincreasedat1C/minfrom35Cto135C. The concentration of the eluted specieswas measured using the instruments built-indifferentialrefractiveindexdetector.Boththe chromatogram and the temperature wererecorded using two data channels and storedusing Millennium 32 software (Waters). Weallowedanadditional40minforcompletecleaning of the column before the next injec-tion.Therefore,thetotaltimeforanalysiswas approximately 6 h, and the system couldperformfiveanalyticaltemperature-risingelutionfractionationsinanautomatedmode.Samplepreparation:Tocheckrepro-ducibility and to calibrate the area versus theconcentration,weusedpolyethylenestan-dardsfromtheNationalInstituteofStan-dards and Technology, denoted polyethyleneNBS1475(linearpolyethylene)andpoly-ethyleneNBS1476(branchedpolyethyl-ene).Thepolymersolutionswerepreparedat 145 C in 1,2,4-trichlorobenzene at 115mg/mLconcentrationswiththeinstru-ments built-in procedure.Results and DiscussionChromatograminterpretation:Todemon-strate how the variation of column tempera-tureaffectsthebaselinestability,Figure1shows two chromatograms of the polyethyl-ene NBS 1475 sample obtained for two con-centrations.Thebaselinesoverlapoutsidetheelutiondomain.Thebaselinedriftiscausedprimarilybythetemperatureandpressure variations in the column during theheating step. To eliminate the drift, we sim-ply used a linear interpolation of the baselineunder the peak.Optimization of injection time: In previ-ouslydescribedmethods,theanalytical Figure1: Analyticaltemperature-risingelu-tion fractionation chromatograms of polyethyl-ene NBS 1475 recorded for two concentrations(3 mg/mL: black line; 6 mg/mL: pink line) show-ingthecontinuousdriftofthebaselinewithelution time.0.200.180.160.14Detector response (mV)Time (min)3 mg/mL6 mg/mL40 50 60 70 80 9056 LCGC NORTH AMERICAVOLUME 22NUMBER 1JANUARY 2004www.chromatographyonline.comtemperature-risingelutionfractionationcolumnwasfilledwithapolymersolu-tionandthenclosedandcooledwitha controlled-temperatureprogram(911).Afterthecrystallizationstep,thecolumnwas reintroduced in the solvent stream.The use of an autoinjector is essential forthepossibilityofacompletelyautomatedprocess,whichimpliesthatthecolumnremains coupled with the high performanceliquidchromatography(HPLC)systemduringbothcoolingandheatingsteps.Therefore, the objective of the injection stepistointroducethesamplecompletelyintothe column and to avoid any spilling of thesamplefromthecolumnwhenthesolventowisstopped.Becauseoftheserequire-ments,itisnecessarytomeasuretheopti-mal injection time in the column.For highly crystalline samples, shorter orlonger injection times will produce the pre-cipitation of the polymer in the inlet or out-let tube, respectively. Because the polyethyl-ene NBS 1476 sample has a lower meltingtemperatureandalsopresentsabroaderrange of elution temperatures, we selected itformeasuringtheoptimalinjectiontime.Thesefeaturesareessentialtopreventobstructionofthecapillarytubeswhenusing short or long injection times. Figure 2illustrates the variation of the ratio betweenthechromatographicareaandtheinjectedmass versus the injection time.Forinjectiontimeslessthan10min,weobserved a domain of almost constant values.For 11 min, a portion of the injected samplespilledintheoutlettubeandwaselutedimmediatelyaftertheowwasrestarted.Because this portion was masked by the sol-ventpeak,theanalyticaltemperature-risingelutionfractionationpeakpresentedasmaller area than expected. Based upon datafrom Figure 2, we selected an injection timeof 9 min.Calibration curve: For quantitative mea-surements of the eluted fractions, we gener-atedacalibrationcurveofthedetectorresponse versus injected mass for polyethyl-eneNBS1475.Figure3presentsthedataobtainedfor117mg/mLconcentrations.The linearity of the data is satisfactory.Reproducibility of elution temperature:Animportantparameterforthequalityofananalyticaltemperature-risingelutionfractionationmethodisthereproducibilityoftheelutiontemperature(volume)foracharacteristicpeak.Theelutiontempera-ture (Tpeak) was taken as the temperature ofthebaththatcorrespondedtothemaxi-mumsignalofthedetector.Tpeakwasrecordedusingtheseconddatachannel.Figure4showstheelutiontemperaturesthat correspond to the peaks of the samplesinjected for the calibration curve presentedin Figure 3.The elution time is reproducible for con-centrationsgreaterthan3mg/mL.Averysmalldecreasecanbedetectedonlyforlowerconcentrations.Figure5illustratesthechromatogramsforthreeinjectedcon-centrations after baseline subtraction.Methodresolution:Thepowerofananalyticaltemperature-risingelutionfrac-tionation method is its ability to resolve dif-ferent polyethylenes that differ by only theirshort-chainbranchingdistribution.Baseduponthelinearrelationshipbetweentheelutiontemperatureandthedegreeofbranching, we can represent the short-chainbranchingdistributionastheweightfrac-tion of the eluted species versus elution tem-peratures.Forthispurpose,wesubtractedthe baseline and normalized the peak.Figure 6 shows the short-chain branchingdistributionsobtainedusingthedescribedanalyticaltemperature-risingelutionfrac-tionation method for the two polyethylenestandards.ThetemperaturedomainsinwhichthepolyethyleneNBS1475andpolyethyleneNBS1476standardsareelutedaresimilarwiththereporteddata forhighlycrystallinepolyethyleneandFigure6: Short-chainbranchingdistribu-tionsfortwotypesofpolyethylenes:linear(polyethyleneNBS1475)andbranched(poly-ethylene NBS 1476).0.250.200.150.100.050.00Short-chain branching (%)Temperature (C)NBS 1476NBS 147560 70 80 90 100 110Figure5: Analyticaltemperature-risingelu-tion fractionation chromatograms of polyethyl-ene NBS 1475 for three injected concentrations(1.01mg/mL:blue;5.37mg/mL:pink;16.38mg/mL: black).0.0400.0300.0200.0100.000Detector response (mV)Temperature (C)1.01 mg/mL5.37 mg/mL16.38 mg/mL60 70 80 90 100 110Figure 4: Variation of the peak elution tem-peratureforpolyethyleneNBS1475asafunc-tionoftheconcentrationofthesamplesolu-tion.97.597.096.596.0Elution temperature (C)Concentration (mg/mL)0 5 10 15 20Figure 3: Calibration curve for polyethyleneNBS1475in1,2,4-trichlorobenzenewithcon-centrations between 1 mg/mL and 17 mg/mL.12.08.04.00.0ADRI ([mVs] 106)Injection mass (mg)R2 0.99920 2 4 6 8Figure2: Variationoftheratiobetweenchromatographic area and injected mass versusinjectiontimeforpolyethyleneNBS1476at 5 mg/mL.1.501.451.401.351.30ADRI/Minj ([mVs/mg] 106)Injection time (min)6 7 8 9 10 11 12JANUARY 2004 LCGC NORTH AMERICAVOLUME 22NUMBER 1 57 www.chromatographyonline.combranchedpolyethylene,respectively(11,18,19).It is important to mention that the reso-lutiondependsuponthetemperaturepro-gram (18). The resolution can be improvedforcomplexsamplesbyusingslowertem-peraturegradientsforbothcrystallizationand elution steps.ConclusionsTodevelopanautomatedanalytical temperature-risingelutionfractionationmethodweneededtwoequallyimportantthings:asuitablecommercialsystem(oraminormodificationofacommercialsys-tem)andareproduciblemethodwiththissystem.In this article, we have presented a simplemethod to obtain an analytical temperature-risingelutionfractionationsystemusingaminor modication of a commercially avail-ableGPCinstrumentandatemperature-programmingsystem.Wealsohaveestab-lishedseveralguidelinesfortheanalyticaltemperature-risingelutionfractionationsys-temqualicationthatusetheacceptedpro-cedure for the validation of chromatographicsystems.An important parameter for the identi-cation of compounds using HPLC systemsis the reproducibility of the elution time fordifferent analyzed compounds. For the ana-lyticaltemperature-risingelutionfractiona-tionmethod,thisreproducibilityistrans-lated into the reproducibility of the elutiontemperature.Usingthesystemdescribedabove,weobtainedareproducibilityof0.05 C for polyethylene NBS 1475 con-centrationsgreaterthan3mg/mLandasgreat as 20 mg/mL.ForquantitativeanalysesofmixturesusingtheHPLCmethods,agoodcalibra-tion curve peak area versus injected mass is essential. In the analytical temperature-risingelutionfractionationmethod,themixtureiscomposedoffractionsthathavedifferentmeltingtemperaturesinsolution.These fractions are recorded as a single chro-matogram, which is used to obtain a short-chainbranchingdistribution.Forthisrea-son,alinearcalibrationcurvemustbeveriedforabroaddomainofconcentra-tionsbeforedeterminationofshort-chainbranchingdistribution.Usingoursystem,wefoundanexcellentlinearcorrelationbetween peak area and injected mass of thepolymerforadomainof0.117mg/mLconcentrations, which provides the possibil-ity of a quantitative determination of short-chain branching distribution.References(1) P.J. Flory, Principles of Polymer Chemistry (Cor-nell University Press, Ithaca, New York, 1953).(2) P.Viville,D.Daoust,A.M.Jonas,B.Nysten,R.Legras,M.Dupire,J.Michel,andG.Debras, Polymer 42, 19531967 (2001).(3) S. Nagano and Y. Goto, J. Appl. Polym. Sci. 26,42174231 (1981).(4) F.M.Mirabella,J.Polym.Sci.BPolym.Phys.39, 28192832 (2001).(5) J. Xu and L. 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