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Handbook of Size Exclusion Chromatography and Related ...

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educed viscosity, h r, to be computed at each instant, without any calibration<br />

factor, according to<br />

h r(t) ¼<br />

V(t) V(0)<br />

V(0)c(t)<br />

The intrinsic viscosity [h] is related to h r according to<br />

h r ¼ [h] þ kH[h] 2 c þ kH,2c 2 þ O(c 3 ) (6)<br />

where kH is 0:4 for neutral polymers, <strong>and</strong> kH,2 has no generally accepted<br />

theoretical form for coil polymers, although empirical expressions exist (30). [h]<br />

measures the hydrodynamic volume VH, per unit mass according to<br />

[h] ¼ 5VH<br />

2M<br />

Shear rates in the capillary viscometer were <strong>of</strong> the order 500s 1 .<br />

1.3 Heterogeneous Time-Dependent Static Light Scattering<br />

(HTDSLS)<br />

Recently, HTDSLS was introduced as a detection <strong>and</strong> analysis technique, in order<br />

to permit the simultaneous characterization <strong>of</strong> solutions containing co-existing<br />

populations <strong>of</strong> polymers <strong>and</strong> colloids (31). Such solutions occur in many contexts:<br />

(1) bacteria that produce or degrade natural products, such as proteins <strong>and</strong><br />

polysaccharides, (2) microgels <strong>and</strong> microcrystals that form inside polymer<br />

reaction solutions, aggregates <strong>of</strong> proteins, <strong>and</strong> other polymers in otherwise<br />

homogeneous solutions, (3) solutions containing “dust” <strong>and</strong> other optical<br />

contaminants that would normally have rendered the solution uncharacterizable by<br />

classical light-scattering techniques. Other scenarios also exist.<br />

The main notion <strong>of</strong> HTDSLS is to make a very small scattering volume Vs<br />

(<strong>of</strong> the order <strong>of</strong> nanoliters, as opposed to the total sample volume, which is<br />

typically tens <strong>of</strong> microliters) <strong>and</strong> to use a flowing sample, so that each time a<br />

colloid particle passes through the scattering volume a large scattering spike is<br />

produced. It has been shown (31) that the “clear window time,” CWT, that is, the<br />

fraction <strong>of</strong> time no large scatterers are in the illuminated scattering volume, has the<br />

limiting form<br />

(5)<br />

(7)<br />

CWT ffi exp( nVs) (8)<br />

where n is the number density <strong>of</strong> large particles. In the meantime, the average<br />

scattering level within the scattering volume is a result <strong>of</strong> the polymeric<br />

population. Built-in algorithms then allow for discriminating <strong>and</strong> counting the<br />

spikes due to colloids, while simultaneously measuring the baseline scattering due<br />

to the polymer. Thus, absolute molecular mass <strong>and</strong> size characterization, <strong>and</strong> its<br />

© 2004 by Marcel Dekker, Inc.

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