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Handbook of Size Exclusion Chromatography and Related ...

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macromolecules may strongly differ from that <strong>of</strong> small molecules. Therefore,<br />

some conclusions on the role <strong>of</strong> adsorption <strong>of</strong> low molecular analytes cannot be<br />

directly applied in HPLC <strong>of</strong> macromolecules.<br />

The schematics <strong>of</strong> polymer adsorption on the solid surface are shown in<br />

Fig. 5. Asimilar picture is valid also for adsorption <strong>of</strong> macromolecules on liquid<br />

(mobile phase)–(quasi) stationary phase interfaces. The extent <strong>of</strong> polymer<br />

adsorption depends both on the affinity <strong>of</strong> macromolecules to the surface <strong>and</strong> the<br />

eluent strength (see also Secs 1<strong>and</strong> 4.2). Weakly adsorbed macromolecules are<br />

attachedtosolidsurfaces<strong>and</strong>tointerfaceswithrelativelyshortparts<strong>of</strong>theirchains<br />

(trains are short, free ends are long, <strong>and</strong> loops are large). As 1increases, trains<br />

become longer while the loops <strong>and</strong> free ends become less frequent <strong>and</strong> their sizes<br />

decrease. To adsorb, macromolecules usually change their conformation (decoiling).<br />

Consequently,adsorption <strong>of</strong> macromolecules is accompanied by large<br />

changes in their conformational entropy.This is one <strong>of</strong> the reasons why extent <strong>of</strong><br />

polymer adsorption may increase with rising temperature <strong>of</strong> the system. Decoiling<br />

<strong>of</strong> macromolecules also allows us to underst<strong>and</strong> adsorption <strong>of</strong> large<br />

macromolecules in narrow pores. At a certain, large 1 value, de-coiled<br />

macromoleculesareabletoreptateintoporesfromwhichtheywouldbeexcluded<br />

in the weak interaction regime (0 1 1cr) (Fig. 6) (15).<br />

It is anticipated that in some systems the summing effect <strong>of</strong> otherwise not<br />

very large segmental interactions may start playing a role at certain molar<br />

masses. As aresult, the calibration dependence would exhibit an unusual backturn<br />

curvature (Fig. 4, curve 10). Wehave also revealed that macromolecules<br />

can penetrate along rather bulky groups bonded on asolid surface to adsorb on<br />

active surface groups (for example, silanols in case <strong>of</strong> silica gel C18 bonded<br />

phase) (16). In this case, polymer adsorption may be limited to rather short<br />

trains or even to single active groups situated on macromolecules. To attain a<br />

measurable change in retention volume, macromolecules must bend <strong>and</strong> attach<br />

on the surface simultaneously with several moieties. This is possible only if<br />

polymer molar mass is high enough <strong>and</strong> therefore the back-turn kink<br />

on calibration dependences affected by adsorption is observed only at a<br />

certain “limiting” size <strong>of</strong> macromolecules. Wespeak about “U-turn adsorption”<br />

(Fig. 7) (15–17). Evidently, conformation <strong>of</strong> this hypothesis will need<br />

Figure 5 Schematic representation <strong>of</strong> macromolecules adsorbed on a solid surface.<br />

© 2004 by Marcel Dekker, Inc.

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