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Self-Assembly of Synthetic and Biological Polymeric Systems of ...

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Additional Supra-<strong>Self</strong>-<strong>Assembly</strong> <strong>of</strong> HSA J. Phys. Chem. B, Vol. 113, No. 36, 2009 12395<br />

Figure 2. (a-c) ESEM images <strong>of</strong> different HSA spherulites incubated at pH 7.4 at 65 °C in the absence <strong>of</strong> added electrolyte along dehydration.<br />

Progressive dehydration allows a better visualization <strong>of</strong> the spherulites. In part c, some surface cracking can be observed. The scale bars are 200,<br />

100, <strong>and</strong> 50 µm in parts a, b, <strong>and</strong> c, respectively. (d) TEM image <strong>of</strong> HSA fibrils obtained after disruption <strong>of</strong> grown spherulites by extensive<br />

sonication.<br />

Figure 3. (a) G′ versus time (cure data) for a 0.8 mM HSA solution<br />

heated at 65 °C atpH(9) 7.4, (b) 2.5, <strong>and</strong> (4) 5.5 in the presence <strong>of</strong><br />

100 mM NaCl. (b) Time evolution <strong>of</strong> storage (G′, O) <strong>and</strong> loss (G′′, 9)<br />

moduli <strong>of</strong> a 0.8 mM HSA solution heated at 65 °C <strong>and</strong> pH 7.4 in the<br />

presence <strong>of</strong> 100 mM NaCl.<br />

biopolymer solution, with the divergence between G′ <strong>and</strong> G′′<br />

becoming larger with time <strong>and</strong> G′′ < G′. Another feature <strong>of</strong><br />

these cure curves is the “dip-down” in the modulus at long times,<br />

which may be indicative <strong>of</strong> slippage <strong>of</strong> the gel samples. 13<br />

Interestingly, G′, though small initially at both pHs, was larger<br />

than G′′ (the loss modulus) even before the gelling point (see<br />

Figure 3b as an example). This “solid-like” behavior <strong>of</strong> the<br />

starting protein solutions has been ascribed to colloid-like<br />

Figure 4. Frequency depedence <strong>of</strong> the storage (G′, closed symbols)<br />

<strong>and</strong> loss (G′′, open symbols) moduli <strong>of</strong> a 0.8 mM HSA solution at pH<br />

(b) 7.4, (9) 2.5, <strong>and</strong> (2) 5.5 in the presence <strong>of</strong> 100 mM NaCl at 65<br />

°C.<br />

structuring in the pregel solution due to nonclassical DLVO<br />

forces. 50,51 This is indicative <strong>of</strong> a different self-assembly<br />

mechanism <strong>and</strong>/or kinetics if compared to what was observed<br />

at pH 5.5, for which G′′ > G′ at short incubation times. At the<br />

latter pH, faster aggregation takes place since enhanced protein/<br />

protein interactions are favored due to the proximity <strong>of</strong> the<br />

solution pH to the protein isoelectric point. It has been pointed<br />

out that rapid formation <strong>of</strong> an appreciable amount <strong>of</strong> intermolecular<br />

-sheets favored by protein/protein interactions 52 involves<br />

very compact structures which precipitate, thereby limiting the<br />

amount <strong>of</strong> protein available to form protein/water networks<br />

necessary for robust gel formation 53 as in the present case. This<br />

fact is also corroborated comparing the lower G′ values at pH<br />

5.5 to those obtained at pH 7.4 <strong>and</strong> 2.5.<br />

Figure 4 shows the corresponding frequency spectrum <strong>of</strong> G′<br />

<strong>and</strong> G′′ for the gels after completion <strong>of</strong> the cure experiment.<br />

Samples at pH 2.5 <strong>and</strong> 7.4 show typical gel spectra. G′ is<br />

179

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