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

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4.3.1.- Relevant aspects<br />

I. For E12S10 dilute solutions, the coexistence <strong>of</strong> spherical micelles with vesicular structures<br />

has been observed. In addition, the spontaneous formation <strong>of</strong> vesicles by<br />

poly(oxystyrene)-poly(oxyethylene) block copolymers is reported for the first time, as<br />

confirmed by light scattering, polarized light microscopy, <strong>and</strong> transmission <strong>and</strong> cryo-<br />

scanning electron microscopy data.<br />

II. In dilute solution, the self-assembly <strong>of</strong> copolymer E10S10E10 leads to the formation <strong>of</strong><br />

elongated micelles as supported by light scattering <strong>and</strong> transmission electron techniques.<br />

III. In the case <strong>of</strong> copolymer E137S18E137, typical spherical micelles are observed. Tube inversion<br />

<strong>and</strong> rheological measurements were used to define the sol- s<strong>of</strong>t- <strong>and</strong> gel-hard boundaries<br />

<strong>of</strong> this copolymer.<br />

IV. E12S10 <strong>and</strong> E10S10E10 copolymers did not form gels in the concentration range analysed.<br />

However, only certain concentrations <strong>of</strong> copolymer E10S10E10 were analysed by rheometry.<br />

From experimental data, an upturn in the low-frequency range <strong>of</strong> the stress moduli was<br />

observed, denoting the existence <strong>of</strong> an emerging slow process, which was assigned to the<br />

formation <strong>of</strong> an elastic network.<br />

V. Block copolymers E12S10, E10S10E10 <strong>and</strong> E137S18E137 showed spontaneous adsorption at the<br />

air-water interface, which slowed down when the hydrophobicity <strong>of</strong> the molecule was<br />

increased. In contrast, at the chlor<strong>of</strong>orm/water interface no measurable effect is observed<br />

for copolymer E12S10 due to the slow diffusion <strong>of</strong> its chains to the interface in combination<br />

with a low bulk concentration; this slow diffusion is associated with the fact that<br />

chlor<strong>of</strong>orm is a good solvent for both E <strong>and</strong> S blocks.<br />

VI. Copolymer E137S18E137 displays an adsorption isotherm with the four classical regions<br />

representing the pancake, mushroom, brush <strong>and</strong> condensed states; the presence <strong>of</strong> a<br />

pseudo-plateau is attributed to the pancake-to-brush transition as E chains submerge into<br />

the aqueous sub-phase. On the other h<strong>and</strong>, for E12S10 <strong>and</strong> E10S10E10 copolymers only two<br />

regions are observed in their adsorption isotherms as a consequence <strong>of</strong> their low<br />

molecular weights, short S <strong>and</strong> E block lengths, <strong>and</strong> much larger S/E ratio. This involves the<br />

disappearance <strong>of</strong> the pseudo-plateau region due to the decrease in the fractional<br />

interfacial area occupied by EO segments.<br />

VII. According to AFM images, circular micelles are observed on Langmuir-Blodgett films <strong>of</strong> the<br />

copolymers obtained at two surface transfer pressures. A decrease in micelle size <strong>and</strong> an<br />

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