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memoria de 2009 - Instituto de Estructura de la Materia - Consejo ...

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POLYMER NANOCOMPOSITES BASED ON CARBON NANOTUBES AND NANOFIBERS<br />

Continuing the work of our group on nanocomposites of technological interest, we have investigated the<br />

conduction mechanisms in a number of systems using a commodity polymer matrix, such as polyethylene, loa<strong>de</strong>d<br />

with carbon based nanoadditives, in particu<strong>la</strong>r, nanofibers and nanotubes. Polymer composites based on<br />

polyami<strong>de</strong> 6,6 (PA66) and different amounts of carbon nanofiber (GANF), supplied by Antolin Ingeniería S.A.,<br />

have been prepared. For this, we have used three different mixing processes: melt compounding, in-situ<br />

polymerization and solvent-ai<strong>de</strong>d mixing. The materials have been characterized morphologically (light<br />

microscopy, SEM) and their thermal (DSC) and electrical (dielectric spectroscopy) properties have been<br />

<strong>de</strong>termined. From preliminary analysis of the results, we conclu<strong>de</strong> that solvent-ai<strong>de</strong>d mixing yields materials with<br />

good dispersion and suitable electrical properties for applications such as electrostatic dissipation, electromagnetic<br />

shielding and electrostatic painting. When the polymerization in situ is carried out, the load is well dispersed in<br />

the matrix and the data indicate that the perco<strong>la</strong>tion threshold has been achieved. However, the materials show<br />

lower conductivity than those composites prepared by solvent-ai<strong>de</strong>d mixing. Finally, melt compounding yields<br />

materials with poor dispersion of nanofibers in the matrix and, in addition, all of them show conductivity values<br />

corresponding to insu<strong>la</strong>ting materials. This fact can be exp<strong>la</strong>ined if we consi<strong>de</strong>r that the nanofibers are broken<br />

during the mixing process and as result, the aspect ratio <strong>de</strong>creases.<br />

BIOPHYSICS: CONFORMATION OF THE MEMBRANE PROTEIN INTEGRINE 2B III<br />

By using X ray and neutron scattering techniques it is possible to obtain information on the conformation of<br />

biological systems, such as proteins in solution. By neutron scattering at low angle, taking advantage of the<br />

possibility of tuning the choice of the contrast between the solvent and protein, we have continued with<br />

experiments to obtain information on the conformations of the integrin α 2b β III complex dissolved in a micelle,<br />

trying to mimic the conformation of the protein when is inserted into the cell membrane. The results can provi<strong>de</strong><br />

some clues about the role and mechanism of action of this protein.<br />

SAXS STUDY ON THE CRYSTALLIZATION OF PET UNDER PHYSICAL CONFINEMENT IN<br />

PET/PC MULTILAYERED FILMS.<br />

The <strong>de</strong>velopment of the crystalline structure of poly(ethylene terephtha<strong>la</strong>te) in multi<strong>la</strong>yered films of poly(ethylene<br />

terephtha<strong>la</strong>te)/polycarbonate (PET/PC) was studied. Films were prepared by the <strong>la</strong>yer multiplying coextrusion<br />

process in the <strong>la</strong>boratory of Prof. E. Baer and Prof A. Hiltner from Case Western Reserve University (Cleve<strong>la</strong>nd,<br />

Ohio, USA). Small angle X-ray scattering (SAXS) patterns were recor<strong>de</strong>d during isothermal crystallization<br />

experiments. At 117C, it was shown that the induction period increases, while the crystallization rate slows down<br />

with increasing <strong>de</strong>gree of physical confinement of PET. On the contrary, the nucleation behaviour is simi<strong>la</strong>r for all<br />

the investigated samples and consequently, it is in<strong>de</strong>pen<strong>de</strong>nt of PET <strong>la</strong>yer thickness. The analysis of the SAXS<br />

curves by means of the Ru<strong>la</strong>nd’s interface distribution function and a dual <strong>la</strong>mel<strong>la</strong>r stack mo<strong>de</strong>l shows that the<br />

<strong>la</strong>mel<strong>la</strong>r stack of PET consists on an average of 3 or 4 corre<strong>la</strong>ted crystals. Structural parameters <strong>de</strong>scribing the<br />

thickness distribution of crystalline, l c , and amorphous phases, l a , of the <strong>la</strong>mel<strong>la</strong>r system were <strong>de</strong>termined. As<br />

expected, l a <strong>de</strong>creases while l c increases during crystallization. When this process comes to an end, those values<br />

are nearly the same for the confined and non-confined PET, which indicates that the formed PET crystals are very<br />

simi<strong>la</strong>r in<strong>de</strong>pen<strong>de</strong>ntly of <strong>la</strong>yer thickness. Finally, the linear crystallinity is found to be much higher than the total<br />

<strong>de</strong>gree of crystallinity obtained by wi<strong>de</strong> angle X-ray experiments (WAXS). This means that not all the volume of<br />

the PET is occupied with stacks of crystals but these stacks are separated by <strong>la</strong>rge amorphous zones in agreement<br />

with earlier findings in non-confined PET.<br />

NANOSTRUCTURE DEVELOPMENT IN POLYMERS BY MEANS OF INDENTATION HARDNESS:<br />

FROM THE GLASSY STATE TO MORE ORDERED STRUCTURES<br />

A review study was un<strong>de</strong>rtaken covering the un<strong>de</strong>rstanding of the nanostructure <strong>de</strong>velopment in g<strong>la</strong>ssy and<br />

semicrystalline polymers as revealed by in<strong>de</strong>ntation hardness methods. The starting point emphasizes the influence<br />

of thermal history and physical ageing on the microhardness of polymer g<strong>la</strong>sses. The corre<strong>la</strong>tion between hardness<br />

and g<strong>la</strong>ss transition temperature T g is brought in. The assumption that microhardness approaches zero for<br />

amorphous materials above T g is experimentally confirmed. A discussion on the influence of filler structure on the<br />

microhardness of polymer g<strong>la</strong>sses is introduced. In<strong>de</strong>ntation hardness is presented as a valuable tool to study the<br />

kinetics of crystallization from the g<strong>la</strong>ssy state and distinct results on polymer systems un<strong>de</strong>r different confinement<br />

conditions are shown. The nanostructure–microin<strong>de</strong>ntation hardness corre<strong>la</strong>tion in the case of semicrystalline<br />

polymers and the influence of <strong>de</strong>gree of crystallinity and crystal thickness for various flexible and semirigid<br />

polymer systems are recalled. Experimental results show that for polymers with low <strong>de</strong>gree of crystallinity and T g<br />

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