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Handbook of Size Exclusion Chromatography and Related ...

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where for species i, Kri ¼ refractometer constant, dn/dc ¼ specific refractive<br />

index increment, <strong>and</strong> c i ¼ concentration. The viscometer provides a signal<br />

proportional to the specific viscosity <strong>of</strong> the sample:<br />

4DP<br />

hsp ¼<br />

(Ip 2DP)<br />

where h sp is the specific viscosity, DP is the differential pressure across the middle<br />

<strong>of</strong> the capillary bridge <strong>of</strong> the viscometer, <strong>and</strong> Ip is the inlet pressure. Thus, at every<br />

elution increment,<br />

DPi ¼ 1<br />

" #<br />

hspi 2 (2 þ hspi) At the very dilute concentrations used in SEC, the intrinsic viscosity at each<br />

increment, [h] i ¼ h spi=ci. Thus, the set <strong>of</strong> data points ci <strong>and</strong> [h]i are collected<br />

across the entire SEC chromatogram. These dilute concentrations also enable<br />

simplification <strong>of</strong> the basic Rayleigh light scattering equation to:<br />

kci<br />

R(Q) i<br />

¼<br />

1<br />

MiP(Q)<br />

where k is a constant dependent upon wavelength, refractive index, dn/dc, <strong>and</strong><br />

R(Q) is the excess Rayleigh scattering factor (2). The P(Q) term approaches unity<br />

for molecules having sizes less than 1/20 <strong>of</strong> the wavelength <strong>of</strong> the incident light.<br />

In TDS, the hydrodynamic radius <strong>of</strong> the molecule, Rh is given by:<br />

Rh ¼ 3 [h]M<br />

p<br />

4 0:025<br />

The radius <strong>of</strong> gyration, Rg, can be determined from the Flory–Fox <strong>and</strong> Ptitsyn–<br />

Eizner equations (8,9):<br />

where,<br />

© 2004 by Marcel Dekker, Inc.<br />

Rg ¼ 1<br />

6<br />

1=2<br />

[h]M<br />

F<br />

F ¼ 2:55 10 21 (1 2:631 þ 2:861 2 ) <strong>and</strong> 1 ¼ (2a 1)=3<br />

Ip<br />

1=3<br />

1=3

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