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Handbook of Size Exclusion Chromatography and Related ...

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which is ameasure <strong>of</strong> the increase in viscosity caused by the addition <strong>of</strong> the<br />

polymer to the solvent. The reduced viscosity h r=c, where cis the polymer<br />

concentration, is ameasure <strong>of</strong> the specific capacity <strong>of</strong> the polymer to increase the<br />

solutionrelativeviscosity.Inthelimit<strong>of</strong> infinitedilutionthisquantityisknownas<br />

the intrinsic viscosity:<br />

[h] ¼ h sp<br />

c c!0<br />

The reduced viscosity has aconcentration dependence in dilute solutions<br />

described by the Huggins equation,<br />

(3)<br />

h sp<br />

c ¼[h]þk0 [h] 2 c (4)<br />

wherek 0 istheHugginsconstant.InSECtheconcentration<strong>of</strong>thesoluteisusually<br />

low,sothattheassumption<strong>of</strong> infinitedilutionisgenerallyvalid<strong>and</strong>theconditions<br />

for Eq. (3) hold. Thus, the intrinsic viscosity <strong>of</strong> an eluting polymer can be<br />

determined from measurements <strong>of</strong> the specific viscosity <strong>and</strong> concentration <strong>of</strong> the<br />

eluting polymer solution at each elution volume.<br />

The intrinsic viscosity <strong>of</strong> apolymer solution is related to its molecular<br />

weight by the empirical relation known as the Mark–Houwink equation:<br />

[h] ¼KM a<br />

whereK<strong>and</strong>aaretheMark–Houwinkcoefficients,whichdependonthepolymer,<br />

solvent, <strong>and</strong> temperature.<br />

Measurement<strong>of</strong>thespecificviscosityrequiresthatboththesolution<strong>and</strong>the<br />

solvent viscosity be measured at the same flow rate. This can be achieved by<br />

measuring the solvent viscosity baseline before <strong>and</strong> after the polymer peak elutes<br />

or by measuring the solution viscosity as the peak elutes using a reference<br />

capillary.Anexample<strong>of</strong>suchaflow-referencedviscometerisshowninFig.1(6).<br />

This is afluid analog <strong>of</strong> the electrical circuit known as aWheatstone bridge. With<br />

onlysolutionflowingthroughtheviscometer,theflowresistancesR1,R2,R3,<strong>and</strong><br />

R4 are balanced <strong>and</strong> the differential pressure transducer signal is zero. When a<br />

polymer solution enters the viscometer, it fills capillaries R1, R2, <strong>and</strong> R3, but the<br />

reservoir prevents it from reaching the fourth capillary,R4, which still contains<br />

flowing solvent. A pressure transducer measures the resultant difference in<br />

pressure between the two sides <strong>of</strong> the bridge. The specific viscosity h sp is<br />

calculatedfromtheratio<strong>of</strong>thisdifferentialpressuretothepressuredropacrossthe<br />

bridge. Other types <strong>of</strong> viscometers include single-capillary (7) <strong>and</strong> referenced<br />

dual-capillary (8) designs. Alisting <strong>of</strong> commercial instrumentation is givenin the<br />

appendix.<br />

Figure 2shows the viscometer <strong>and</strong> refractometer tracings as afunction <strong>of</strong><br />

elution volume for a mixture <strong>of</strong> equal amounts <strong>of</strong> three nearly monodisperse<br />

© 2004 by Marcel Dekker, Inc.<br />

(5)

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