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Handbook of Size Exclusion Chromatography and Related ...

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Figure 1 Chromatogram showing SE/HdC separation <strong>of</strong> narrow polydispersity<br />

polystyrene st<strong>and</strong>ards. Column: two 300 7:5mm PLgel Mixed-E columns in series;<br />

flow rate, 1.0mL/min. A ¼ 4,000,000; B ¼ 1,550,000; C ¼ 550,800; D ¼ 156,000;<br />

E ¼ 66,000; F ¼ 30,300; G ¼ 9200; H ¼ 3250; J–Q ¼ oligomers; R ¼ 162; S ¼ toluene.<br />

(From Ref. 1.)<br />

2 HYDRODYNAMIC CHROMATOGRAPHY<br />

The basic principles <strong>of</strong> HdC are easily explained by considering the transport <strong>of</strong><br />

spherical macromolecules in laminar flow through an open microcapillary tube<br />

(Fig. 3). The solvent velocity pr<strong>of</strong>ile in an open tubular tube is aparabolic<br />

Poiseuille flow.Macromolecules are considered as rigid spheres <strong>and</strong> are neutrally<br />

buoyant. As a result <strong>of</strong> Brownian motion, macromolecules will disperse<br />

throughout the capillary cross-section. Because <strong>of</strong> their finite sizes, the centers <strong>of</strong><br />

thepolymermoleculescannotapproachthecolumnwallanycloserthantheirown<br />

radii. Owing to the fluid velocity pr<strong>of</strong>ile, alarger solute molecule travels through<br />

thecapillaryatagreateraveragevelocitythanasmallersolute.Inotherwords,the<br />

separation <strong>of</strong> HdC is not due to size exclusion itself, but to the faster average<br />

© 2004 by Marcel Dekker, Inc.

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