Estudi dels mecanismes mecànico-químics de la fibrogènesi pulmonar

La fibrosi pulmonar idiopàtica (FPI) és una malaltia intersticial letal, d'etiologia desconeguda i per la que no es disposa de cap tractament efectiu. Creiem que l’elasticitat normal del pulmó té propietats anti-fibròtiques, de manera que la FPI només progressarà si es produeix un enduriment sostingut del teixit. Per això hem dissenyat dos assaigs que ens permetran examinar els efectes pro-fibròtics de l'enduriment extracel•lular sobre fibroblasts primaris de pulmó. Els dos assaigs d'enduriment es basen en gels de poliacrilamida 2D i en gels de col•lagen 3D. Els fibroblasts s'han cultivat en el model d'enduriment 3D en presència o absència de la citoquina pro-fibròtica TGF-β1 i s'ha analitzat com la combinació de l’enduriment extracelular i la TGF-b1 modifiquen el fenotip de les cèl.lules. Els resultats preliminars mostren canvis en l'expressió d'alguns gens en resposta a l'enduriment i al TGF-b1, així com diferències entre cel•lules normals i fibròtiques. A més, suggereixen que l'expressió de COL1A1 i MMP-1 és mecanosensible, i que la seva desregulació podria estar associada a l’enduriment anòmal característic dels pulmons amb FPI.

Avalanche dynamics of fiber bundle models

We present a detailed analytical and numerical study of the avalanche distributions of the continuous damage fiber bundle model CDFBM . Linearly elastic fibers undergo a series of partial failure events which give rise to a gradual degradation of their stiffness. We show that the model reproduces a wide range of mechanical behaviors. We find that macroscopic hardening and plastic responses are characterized by avalanche distributions, which exhibit an algebraic decay with exponents between 5/2 and 2 different from those observed in mean-field fiber bundle models. We also derive analytically the phase diagram of a family of CDFBM which covers a large variety of potential avalanche size distributions. Our results provide a unified view of the statistics of breaking avalanches in fiber bundle models

Magnetic hardening mechanisms in Nd-Fe-B nanocrystalline material

Microstructural and magnetic measurements of the evolution by heat treatment of initially amorphous Nd16Fe76B8 alloys prepared by melt spinning are presented. Evidence of magnetic hardening above a threshold temperature induced by magnetic isolation of the Nd2Fe14B grains is provided. A thermodynamic and kinetic explanation of local melting of the intergranular nanostructured Nd¿rich eutectic phase at temperatures below 900 K based on capillary effects is presented. A subsequent Ostwald ripening process moves Nd to wet intimately the hard magnetic grains, becoming, on cooling, a real paramagnetic isolating thin film (~2.5 nm). By using a simple analogy, it is shown that the switching magnetization field in a single¿domain crystal can be drastically affected through the exchange coupling to neighboring grains with different orientation of the easy axis. This effect should be important enough to reinforce the coercive field of polycrystalline hard magnetic materials and explains the observed enhancement from 0.9 to 1.9 T.

Atomic Ordering and Martensitic Transitions in Cu-Zn-Al Shape Memory Alloys

We present results from both, calorimetric and dilatometric studies of the isothermal ordering process taking place in a Cu-Zn-Al shape memory alloy after quenches from Tq temperatures ranging from 350 K to 1200 K. The dissipated energy and the length variations of the system are obtained during the process. The change of these quantities in the whole process have been compared with the difference [MATH] between Ms, measured after the relaxation and Ms measured just after the quench. We obtain that these three quantities present, as a function of Tq, the same qualitative behaviour. These changes are then associated with changes of the L21 ordering after the quench in the system. The relaxational process does not follow a single exponential decay. Instead, a continuous slowing down is observed. A relaxation time [MATH] has been defined to characterize the relaxation rate. We show that [MATH] depends on both the annealing and the quenching (Tq [MATH] 800 K) temperatures through an Arrhenius law.