[Femoral-venous catheterization: a delayed perforation]. / Cathétérisme veineux fémoral: cas d'une perforation secondaire.

Later vascular injury after central venous catheterization is not common. In literature, there are only cases reporting jugular or subclavian vein catheterization territories with a higher significative risk if the catheter is larger and in left position. We report a case of inferior vena cave perforation, nine days following femoral vein catherization for parenteral nutrition in a 72-year-old patient. This vascular perforation induced an infusion in the peritoneal and the retroperitoneal cavity with abdominal and pelvic pain. This case report may ask the question of recommendations about femoral catherization.

Effects of confinement on freezing and melting.

We present a review of experimental, theoretical, and molecular simulation studies of confinement effects on freezing and melting. We consider both simple and more complex adsorbates that are confined in various environments (slit or cylindrical pores and also disordered porous materials). The most commonly used molecular simulation, theoretical and experimental methods are first presented. We also provide a brief description of the most widely used porous materials. The current state of knowledge on the effects of confinement on structure and freezing temperature, and the appearance of new surface-driven and confinement-driven phases are then discussed. We also address how confinement affects the glass transition.

Confinement of molecular liquids: consequences on thermodynamic, static and dynamical properties of benzene and toluene.

We relate the dynamical behavior of molecular liquids confined in mesoscopic cylindrical pores to the thermodynamic properties, heat capacity and density and to the static structure by combining different experimental methods (H-NMR, calorimetry, elastic and inelastic neutron scattering, numerical simulations). The crystallization process is greatly reduced or avoided by confinement under standard cooling conditions, instead a glass transition temperature T(g) at the 1000s time scale can be observed. The pore averaged local structure of the confined liquid is not noticeably affected when "excluded-volume" corrections are carefully applied, but follows the density changes reflected by the Bragg peak intensities of the porous matrices. The pore size dependence of T(g) is dominated by two factors, surface interaction and finite-size effect. For the smallest pores ([Formula: see text], [Formula: see text] being the van der Waals radius of a molecule), one observes an increase of T(g) and a broadening of the transition region, related to the interaction with the surface that induces a slowing-down of the molecules close to the wall. This is confirmed by neutron scattering experiments and molecular-dynamics simulations at shorter time scales and higher temperatures, which indicate a remaining fraction of frozen molecules. For larger pore sizes, taking the decrease of density under confinement conditions into account, a decrease of T(g) is observed. This could be related to finite-size effects onto the putative cooperativity length that is often invoked to explain glass formation. However, no quantitative determination of this length (not to mention its T-dependence) can be extracted, since the interaction with the wall itself introduces an additional length that adds to the complexity of the problem.

Methyl group dynamics in a confined glass.

We present a neutron scattering investigation on methyl group dynamics in glassy toluene confined in mesoporous silicates of different pore sizes. The experimental results have been analysed in terms of a barrier distribution model, such a distribution following from the structural disorder in the glassy state. Confinement results in a strong decreasing of the average rotational barrier in comparison to the bulk state. We have roughly separated the distribution for the confined state in a bulk-like and a surface-like contribution, corresponding to rotors at a distance from the pore wall respectively larger and smaller than the spatial range of the interactions which contribute to the rotational potential for the methyl groups. We have estimated a distance of 7 A as a lower limit of the interaction range, beyond the typical nearest-neighbour distance between centers-of-mass (4.7 A).