Thickening of phase change materials (PCM) to avoid segregation

Estudi elaborat a partir d’una estada a Çukurova University, Turquia, al juliol del 2006. L’emmagatzematge d’energia tèrmica ha atret interès en aplicacions tèrmiques com l’aigua calenta, la calefacció i l’aire condicionat. Aquests sistemes són útils per corregir la no coincidència entre la oferta i la demanda d’energia. Principalment hi ha dos tipus de sistemes d’emmagatzematge d’energia tèrmica, emmagatzematge amb calor sensible i amb calor latent. L’emmagatzematge amb calor latent és particularment atractiu degut a la seva habilitat de donar una densitat d’emmagatzematge d’energia més alt i la seva característica d’emmagatzemar calor a una temperatura constant corresponent a la temperatura de transició de fase de la substància emmagatzemadora de calor. Les salts hidratades orgàniques tenen certes avantatges com a materials d’emmagatzematge de calor latent sobre els materials orgànics. En canvi, quan les salts hidratades s’utilitzen com a materials de canvi de fase (PCM) apareixen alguns problemes en les aplicacions d’emmagatzematge de calor latent. Aquests són el subrefredament de les salts hidratades quan es congelen degut a les seves dèbils propietats de nucleació, i la separació de fase que hi apareix degut a una fusió incongruent. En aquest estudi, s’estabilitza sal de Glauber (Na2SO4.10H2O) amb diferents concentracions de poliacrilamida i gelatina per prevenir la fusió incongruent. Per prevenir el subrefredament s’utilitza un agent nucleant amb una estructura cristal•lina semblant a la de la sal de Glauber. La capacitat d’emmagatzematge de calor de les mostres de PCM estabilitzades amb diferents concentracions de gels polimèrics es determinen amb DCS i amb el mètode T-history.

Nuevos carboranil alcoholes que contienen anillos aromáticos nitrogenados: síntesis, caracterización, análisis estructural y estudios preliminares de reactividad

Se han sintetizado nueve alcoholes que incorporan diversos isómeros de los grupos piridil o quinolil y metil-o-carborano u o-carborano, 1-[n′-Piridil(hidroxi)metil]-2-R-1,2-dicarba-closo-dodecaboranos (n′ = 2, R = H (2a); n′ = 3, R = Me (1c) y H (2c)), 1-[2′-6-metil-piridil(hidroxi)metil]-2-R-1,2-dicarba-closo-dodecaboranos (R = Me (1b) y H (2b)), 1-[n′-Quinolil(hidroxi)metil]-2-R-1,2-dicarba-closo-dodecaboranos (n′ = 2, R = Me (1e) y H (2e); n′ = 4, R = Me (1f) y H (2f), mediante la adición de la sal de litio del metil-o-carborano u o-carborano a los aldehídos correspondientes. Los compuestos se han obtenido con rendimientos altos en la mayoría de los casos y han sido caracterizados mediante Resonancia Magnética Nuclear, por Espectroscopía Infrarroja y análisis elemental. Las estructuras cristalinas de siete de los nueve compuestos (1c, 1f, 2a, 2b, 2c, 2e y 2f) se han determinado mediante Cristalografía por Rayos X. Se han analizado las estructuras cristalinas de los todos los compuestos y se han comparado con las estructuras de los compuestos relacionados 1a, 1b, y 2a, obtenidas previamente en el grupo de Síntesis Inorgánica y Catálisis del ICMAB. Todas las estructuras muestran interacciones por puentes de hidrógeno O–H···N moderadamente fuertes. Posteriormente se ha sintetizado el derivado mesilado 4 (derivado del o-carborano) mediante la reacción del alcohol 2a con cloruro de mesitilo a temperatura ambiente, con rendimiento alto. El nuevo mesilato 4 se ha caracterizado mediante Resonancia Magnética Nuclear. El nuevo mesilato resulta un compuesto de partida muy versátil para la síntesis de nuevos derivados mediante la substitución del grupo mesilo por nucleófilos apropiados, como por ejemplo las aminas. El grupo ha publicado recientemente la síntesis de diaminas mediante la reacción de substitución del mesilato relacionado 3 (derivado del metil-o-carborano) con aminas, entre ellas la bencilamina. Se ha realizado por tanto la reacción de substitución del grupo mesilato en 4 por la bencilamina para obtener la diamina correspondiente. Los resultados preliminares de esta reacción muestran que si bien el grupo mesilato en 4 ha sido substituido, el clúster se degrada casi en su totalidad a un derivado tipo nido. Esto contrasta claramente con la reactividad del mesilato análogo 3 frente a la bencilamina, ya que en este caso se obtiene la diamina deseada y el clúster no se degrada apreciablemente bajo las mismas condiciones de reacción. Se han realizado estudios preliminares por RMN que muestran que la bencilamina substituye al grupo mesilo en 4 y posteriormente el clúster closo se degrada a una especie nido que no ha sido posible caracterizar totalmente hasta el momento.

C-H···O H-bonded complexes: how does basis set superposition error change their potential-energy surfaces?

Geometries, vibrational frequencies, and interaction energies of the CNH⋯O3 and HCCH⋯O3 complexes are calculated in a counterpoise-corrected (CP-corrected) potential-energy surface (PES) that corrects for the basis set superposition error (BSSE). Ab initio calculations are performed at the Hartree-Fock (HF) and second-order Møller-Plesset (MP2) levels, using the 6-31G(d,p) and D95++(d,p) basis sets. Interaction energies are presented including corrections for zero-point vibrational energy (ZPVE) and thermal correction to enthalpy at 298 K. The CP-corrected and conventional PES are compared; the unconnected PES obtained using the larger basis set including diffuse functions exhibits a double well shape, whereas use of the 6-31G(d,p) basis set leads to a flat single-well profile. The CP-corrected PES has always a multiple-well shape. In particular, it is shown that the CP-corrected PES using the smaller basis set is qualitatively analogous to that obtained with the larger basis sets, so the CP method becomes useful to correctly describe large systems, where the use of small basis sets may be necessary

Reduction of symmetry in grandite solid solution

The results of a crystal structure refinement of an anisotropic grandite garnet specimen with composition Gro36-4 And63-6 are given. The structure obtained has orthorrombic symmetry (space group Fddd) and is compared with similar results obtained by other authors. In all cases the reduction of symmetry is due to the ordering of Fe3+ and Al in octahedral sites. Non cubic structures of grandites are discussed in connection with optical, morphological an grou-th features of these minerals.

Estudio cuantitativo de la reacción en estado sólido del fluorapatito

Mediante difracción de rayos X se valora cuantitativamente el fluoruro cálcico remanente en la reacción al estado sólido con hidroxiapatito, para formar fluorapatito, a distintos tiempos y temperaturas de tratamiento térmico. Se observa que tanto el aumento de temperatura como el tiempo de calefacción hacen descender el porcentaje de fluoruro cálcico libre, que por otra parte siempre está presente, por cuanto la reacción no es total.

Sistema automático para determinar estructuras cristalinas por difracción de rayos-X

Se desarrolla en este trabajo un sistema de calculo para la determinación de estructuras cristalinas por difracción de rayos-X. Las caracteristicas de este sistema son: Incorporar los métodos y las técnicas más recientes. Obtener la máxima velocidad de ejecución posible. Obtener la total automatización del proceso. Y conseguir la mínima ocupacion de memoria posible.

Cation distribution and magnetization of BaFe12-2xCoxSnxO19 (x=0.9,1.28) single crystals

The distribution of Sn4+ cations within the five crystallographic sites of the magnetoplumbite (M) ‐like compound BaFe12−2xCoxSnxO19 has been analyzed using single‐crystal x‐ray‐diffraction data. The species Fe3+ and Co2+ cannot be distinguished using x rays because of their very similar atomic numbers; however, the calculation of the apparent valencies for the different sites allows an insight into the Co2+ cation segregation. The use of previous data from neutron powder diffraction allows a precise picture of the cation distribution, which indicates a pronounced site selectivity for both Sn4+ and Co2+ cations. The Sn4+ cations prefer the 4f2 sites and to a much lower extent the 12k sites, while they do not enter the octahedral 2a sites at all. Co2+ cations are distributed among tetrahedral and octahedral sites displaying a clear preference for the tetrahedral 4f1 sites. Magnetic measurements indicate that the compound still exhibits uniaxial anisotropy with the easy direction parallel to the c axis. Nevertheless, the magnetic structure shows a considerable degree of noncolinearity. A strong reduction of the magnetic anisotropy regarding that of the undoped compound is also detected.

A simple method for the simulation of multiple elastic scattering of electrons

A screened Rutherford cross section is modified by means of a correction factor to obtain the proper transport cross section computed by partial¿wave analysis. The correction factor is tabulated for electron energies in the range 0¿100 keV and for elements in the range from Z=4 to 82. The modified screened Rutherford cross section is shown to be useful as an approximation for the simulation of plural and multiple scattering. Its performance and limitations are exemplified for electrons scattered in Al and Au.

Monte Carlo simulation of kilovolt electron transport in solids

A Monte Carlo procedure to simulate the penetration and energy loss of low¿energy electron beams through solids is presented. Elastic collisions are described by using the method of partial waves for the screened Coulomb field of the nucleus. The atomic charge density is approximated by an analytical expression with parameters determined from the Dirac¿Hartree¿Fock¿Slater self¿consistent density obtained under Wigner¿Seitz boundary conditions in order to account for solid¿state effects; exchange effects are also accounted for by an energy¿dependent local correction. Elastic differential cross sections are then easily computed by combining the WKB and Born approximations to evaluate the phase shifts. Inelastic collisions are treated on the basis of a generalized oscillator strength model which gives inelastic mean free paths and stopping powers in good agreement with experimental data. This scattering model is accurate in the energy range from a few hundred eV up to about 50 keV. The reliability of the simulation method is analyzed by comparing simulation results and experimental data from backscattering and transmission measurements.

Simple method for the simulation of multiple elastic scattering of electrons

A screened Rutherford cross section is modified by means of a correction factor to obtain the proper transport cross section computed by partial¿wave analysis. The correction factor is tabulated for electron energies in the range 0¿100 keV and for elements in the range from Z=4 to 82. The modified screened Rutherford cross section is shown to be useful as an approximation for the simulation of plural and multiple scattering. Its performance and limitations are exemplified for electrons scattered in Al and Au.

Computer simulation study of liquid lithium at 470 and 843 K

Both structural and dynamical properties of 7Li at 470 and 843 K are studied by molecular dynamics simulation and the results are comapred with the available experimental data. Two effective interatomic potentials are used, i.e., a potential derived from the Ashcroft pseudopotential [Phys. Lett. 23, 48 (1966)] and a recently proposed potential deduced from the neutral pseudoatom method [J. Phys.: Condens. Matter 5, 4283 (1993)]. Although the shape of the two potential functions is very different, the majority of the properties calculated from them are very similar. The differences among the results using the two interaction models are carefully discussed.

Static and dynamic structure of liquid metals: Role of the different parts of the interaction potential

The influence of different parts of the interaction potential on the microscopic behavior of simple liquid metals is investigated by molecular dynamics simulation. The role of the soft-core repulsive, short-range attractive, and long-range oscillatory forces on the properties of liquid lithium close to the triple point is analyzed by comparing the results from simulations of identical systems but truncating the potential at different distances. Special attention is paid to dynamic collective properties such as the dynamic structure factors, transverse current correlation functions, and transport coefficients. It is observed that, in general, the effects of the short-range attractive forces are important. On the contrary, the influence of the oscillatory long-range interactions is considerably less, being the most pronounced for the dynamic structure factor at long wavelengths. The results of this work suggest that the influence of the attractive forces becomes less significant when temperature and density increase.