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12394 J. Phys. Chem. B, Vol. 113, No. 36, 2009 Juárez et al.<br />

Figure 1. (a) Optical microscopy images <strong>of</strong> grown spherulites <strong>of</strong> HSA at pH 7.4 in the absence <strong>of</strong> added NaCl at 65 °C after 72 h <strong>of</strong> incubation<br />

under cross-polarizers. The inset indicates the radial arrangement <strong>of</strong> fibrils through insertion <strong>of</strong> a waveplate at 45° between the polarizers. (b)<br />

Fluorescence image in the confocal mode <strong>of</strong> spherulites using ThT as a probe. (c) Confocal image in the transmission mode <strong>of</strong> spherulites between<br />

cross-polarizers. (d) ThT fluorescence upon incubation in a solution without HSA, containing native HSA <strong>and</strong> containing spherulites. (e) Optical<br />

microscopy image <strong>of</strong> HSA spherulites without polarizers. Scale bars are (a) 50, (b) 200, <strong>and</strong> (c <strong>and</strong> e) 100 µm.<br />

outer edges <strong>of</strong> the spherulites, where the fibril bundles are<br />

slightly separated from one another.<br />

The spherical morphology <strong>of</strong> spherulites was also observed<br />

by ESEM (see Figure 2), with sizes similar to those derived<br />

from optical <strong>and</strong> confocal microscopy. Their surface appears<br />

to have a texture on the length scale <strong>of</strong> several micrometers<br />

but shows no obvious orientational order. Some cracks on the<br />

particle surface appeared as a consequence <strong>of</strong> the dehydration<br />

process in ESEM. Unfortunately, we could not observe if the<br />

spherulites formed display a radial internal order, since internal<br />

cracking <strong>of</strong> spherulitic structures was not achieved.<br />

Direct measurement <strong>of</strong> spherulitic solutions was not posible<br />

by TEM provided that a film was formed on the grids which<br />

do not allow visualization. In this way, dilution <strong>and</strong> sonication<br />

<strong>of</strong> the spherulitic solutions were performed in order to investigate<br />

the samples by TEM. This treatment resulted in the<br />

disruption <strong>of</strong> the spherulites <strong>and</strong> the appearance <strong>of</strong> amyloidlike<br />

fibril structures, as seen in Figure 2d. This fact further<br />

confirms that spherulites are mainly composed <strong>of</strong> amyloid fibrils.<br />

Gel Formation <strong>and</strong> Characterization. Prolonged incubation<br />

<strong>of</strong> solutions containing 0.3 mM HSA (or 0.8 mM where<br />

corresponds) at either pH 7.4, 5.5 or 2.5 at 65 °C in the presence<br />

<strong>of</strong> different amounts <strong>of</strong> added salt leads to the formation <strong>of</strong><br />

gels. In this work, we have only analyzed solution conditions<br />

previously studied for amyloid fibril formation. 41,42 Significant<br />

differences were observed in the association properties <strong>of</strong> the<br />

different protein solutions. In this way, we have observed that<br />

at pH 7.4 <strong>and</strong> 5.5 gels were formed at electrolyte concentrations<br />

larger than 20 mM with gelation times decreasing from several<br />

days to hours as the solution ionic strength increases (or the<br />

protein concentration rises). On the other h<strong>and</strong>, under acidic<br />

conditions gels were only formed at the highest electrolyte<br />

concentration analyzed, 250 mM NaCl at 0.3 mM HSA. In<br />

general, it seems that gel formation is favored by the screening<br />

<strong>of</strong> electrostatic interactions between protein molecules, which<br />

favors protein aggregation. 45,46 Nevertheless, protein interactions<br />

at acidic pH are weaker than those at physiological pH due to<br />

the initial different conformational state <strong>of</strong> the protein (Exp<strong>and</strong>ed-E<br />

state under acidic conditions), which imparts a larger<br />

solubility to the acid-denaturated protein molecules as a result<br />

<strong>of</strong> electrostatic repulsion between them due to an increase <strong>of</strong><br />

surface-charged groups.<br />

Figure 3a shows cure curves (G′, the storage modulus, versus<br />

time) for gelling HSA solutions at pH 7.4, 5.5, <strong>and</strong> 2.5 in the<br />

presence <strong>of</strong> 100 mM NaCl at 65 °C. To follow the protein<br />

gelation in a suitable time scale for the experiment, we increased<br />

the protein concentration up to 0.8 mM. The obtained cure data<br />

are typical <strong>of</strong> a sol-gel transition <strong>of</strong> biopolymer solutions: The<br />

elastic component <strong>of</strong> the shear modulus starts small but<br />

undergoes a sudden increase at a critical time <strong>and</strong>, then,<br />

ultimately almost levels <strong>of</strong>f at longer times. For pH 7.4 <strong>and</strong><br />

2.5, the behavior is similar to that expected for a strongly gelling<br />

178

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