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Chapt4MolecularWeightandMolecularWeightDistributionofPolymers4.1高聚物分子量和分子量分布的表示方法4.2分子量的测定方法4.3分子量分布的测定方法4.2.1数均分子量的测定方法4.2.2重均分子量的测定方法4.2.3粘均分子量的测定方法MolecularweightandmolecularweightdistributionDistributionofmolecularweightsinatypicalpolymer4.1DefinitionsofAverageMWsandMWDistributionn:totalmolenumber;ni:molenumberofithmoleculewithmolemassofMi;Ni:molefractionofithmolecule;w:totalweightofthesample;wi:weightoftheithmolecule;Wi:weightfractionofithmolecule.(1)Number-averagemolecularweight(数均分子量):(2)Weight-averagemolecularweight(重均分子量):SchulzTungLogarithmnormaldistribution用简化的函数拟合MWDistribution

Widthofmolecularweightdistribution(分子量分布宽度):Polydispersity(多分散系数):MWDistributionFunction实验测量平均分子量分布宽度4.2MeasurementofMolecularWeight

Endgroupanalysis(端基分析)molecularweightdeterminationthroughgroupanalysisrequiresthatthepolymercontainaknownnumberofdeterminablegroupspermolecule.measurethenumber-averagemolecularweight,Mn

2.5104

Colligativeproperty(依数性)measurement:

measurethenumber-averagemolecularweightMnvapor-pressurelowingboiling-pointelevation(ebulliometry)freezing-pointdepression(cryoscopy)osmoticpressure(osmometry)DTb,DTf,andParetheboiling-pointelevation,freezing-pointdepression,andosmoticpressure.risthedensityofthesolvent.DHvandDHfaretheenthalpiesofvaporizationandfusion.

Vapor-phaseosmometry(VPO,气相渗透法)Smalltemperaturedifferenceresultingfromdifferentratesofsolventevaporationfromandcondensationontodropletsofpuresolventandpolymersolutionmaintainedinanatmosphereofsolventvapor.MeasureMnthatistoolowerformembraneosmometrymethod.Calibratedwithlow-molecularweightstandards:arelativemethod.Quasi-steady-statephenomena.caremustbetakentostandarizesuchvariablesastimeofmeasurementanddropsizebetweencalibrationandsamplemeasurement.MeasurementchamberofVPO(Pasternak,1962).Dropletsofsolventandpolymersolutionareplaced,withtheaidofhypodemicsyringer,onthe“beads”oftwotheristorsusedastemperature-sensingelementsandmaintainedinequilibriumwithanatmosphereofsolventvapor.

Membraneosmometry(膜渗透压法)DiagramoftheZimm-myersonosmometer(Zimm1946).Atypicaldiameterforthemeasuringandreference(solventcell)capillaryis0.5-1mm.Theclosureofthefillingtubeisa2-mmmetalrod.Amercurysealisusedatthetoptoensuretightness.TwomembraneareheldagainstaglasssolutioncellbymeansofperforatedmetalplatesTheassembledinstrumentissuspendedinalargetubepartlyfilledwithsolventThesuccessoftheosmoticexperimentdependsontheavailabilityofamembranethroughwhichsolventbutnotsolutemoleculescanpassfreely.Existingmembranesonlyapproximatelyidealsemipermeability.Measurablemolecularweight:2104<Mn<106.

Staticlightscattering(静态光散射)Generalset-upofascattering(散射)experimentIncidentbeamIntensityI0ScatteredbeamIntensityI(q)DetectorSampleScatteringvector(散射矢量):where:wavelengthoftheradiationqTheoryofLightScatteringRandomPhaseApproximationbydeGennesForpolymer/polymermixtureForPolymerSoultiong:

StructurefactorofasinglechainA:PolymerB:Solvent(Rayleighratio)瑞利比(2)largeparticlesd>l/20qrI0II

µ(SAi)2q→0cY斜率2A2sin2q/2c1c2c3Ycq1q2q3YY斜率sin2q/2

TheZimm-Plot2A21/MwSmallanglelaserlightscatteringq»0用光陷阱扣除中心光的干扰Nomenclature(术语)ofsolutionviscosityhr:粘度比(相对粘度);hsp:粘度相对增量(增比粘度);hred:粘数(比浓粘度);hinh:对数粘数(比浓对数粘度);[h]:极限粘数(特性粘度)h:viscosityofpolymersolutionattemperatureTh0:viscosityofpuresolventatT.ViscositymeasurementThesmallmolecularliquidsanddilutepolymersolutionsareNewtonianflow:theviscositydoesnotchangewiththeshearstressandshearrate。Measurementsofsolutionviscosityareusuallymadebycomparingtheeffuxtimet(流出时间)requiredforaspecifiedvolumeofpolymersolutiontoflowthroughacapillary(毛细管)tubewiththecorrespondingeffuxtimet0ofthepuresolvent.IfB/tismuchsmallthanAtandr

r0

TreatmentofviscositydataHugginsequation:Ifhsp<1,hrcanbeexpressedbyTaylorseriesexpansion

Mark-Houwinkequation:Viscosity-averagemolecularweight(粘均分子量):MolecularWeightFractionations(分子量分级)ofPolymers

Columnelution(柱淋洗)Solvent-gradientelution(溶剂梯度淋洗)Thermal-gradientelution(温度梯度淋洗)HighTemp.LowTemp.GoodSolventPoorSolvent

Gelpermeationchrom

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