Selective area growth of a- and c-plane GaN nanocolumns by molecular beam epitaxy using colloidal nanolithography

Selective area growth of a-plane GaN nanocolumns by molecular beam epitaxy was performed for the first time on a-plane GaN templates. Ti masks with 150 nm diameter nanoholes were fabricated by colloidal lithography, an easy, fast and cheap process capable to handle large areas. Even though colloidal lithography does not provide a perfect geometrical arrangement like e-beam lithography, it produces a very homogeneous mask in terms of nanohole diameter and density, and is used here for the first time for the selective area growth of GaN. Selective area growth of a-plane GaN nanocolumns is compared, in terms of anisotropic lateral and vertical growth rates, with GaN nanocolumns grown selectively on the c-plane

Wheel-Rail Contact Forces in High-Speed Simply Supported Bridges at Resonance

The response of high-speed bridges at resonance, particularly under flexural vibrations, constitutes a subject of research for many scientists and engineers at the moment. The topic is of great interest because, as a matter of fact, such kind of behaviour is not unlikely to happen due to the elevated operating speeds of modern rains, which in many cases are equal to or even exceed 300 km/h ( [1,2]). The present paper addresses the subject of the evolution of the wheel-rail contact forces during resonance situations in simply supported bridges. Based on a dimensionless formulation of the equations of motion presented in [4], very similar to the one introduced by Klasztorny and Langer in [3], a parametric study is conducted and the contact forces in realistic situations analysed in detail. The effects of rail and wheel irregularities are not included in the model. The bridge is idealised as an Euler-Bernoulli beam, while the train is simulated by a system consisting of rigid bodies, springs and dampers. The situations such that a severe reduction of the contact force could take place are identified and compared with typical situations in actual bridges. To this end, the simply supported bridge is excited at resonace by means of a theoretical train consisting of 15 equidistant axles. The mechanical characteristics of all axles (unsprung mass, semi-sprung mass, and primary suspension system) are identical. This theoretical train permits the identification of the key parameters having an influence on the wheel-rail contact forces. In addition, a real case of a 17.5 m bridges traversed by the Eurostar train is analysed and checked against the theoretical results. The influence of three fundamental parameters is investigated in great detail: a) the ratio of the fundamental frequency of the bridge and natural frequency of the primary suspension of the vehicle; b) the ratio of the total mass of the bridge and the semi-sprung mass of the vehicle and c) the ratio between the length of the bridge and the characteristic distance between consecutive axles. The main conclusions derived from the investigation are: The wheel-rail contact forces undergo oscillations during the passage of the axles over the bridge. During resonance, these oscillations are more severe for the rear wheels than for the front ones. If denotes the span of a simply supported bridge, and the characteristic distance between consecutive groups of loads, the lower the value of , the greater the oscillations of the contact forces at resonance. For or greater, no likelihood of loss of wheel-rail contact has been detected. The ratio between the frequency of the primary suspension of the vehicle and the fundamental frequency of the bridge is denoted by (frequency ratio), and the ratio of the semi-sprung mass of the vehicle (mass of the bogie) and the total mass of the bridge is denoted by (mass ratio). For any given frequency ratio, the greater the mass ratio, the greater the oscillations of the contact forces at resonance. The oscillations of the contact forces at resonance, and therefore the likelihood of loss of wheel-rail contact, present a minimum for approximately between 0.5 and 1. For lower or higher values of the frequency ratio the oscillations of the contact forces increase. Neglecting the possible effects of torsional vibrations, the metal or composite bridges with a low linear mass have been found to be the ones where the contact forces may suffer the most severe oscillations. If single-track, simply supported, composite or metal bridges were used in high-speed lines, and damping ratios below 1% were expected, the minimum contact forces at resonance could drop to dangerous values. Nevertheless, this kind of structures is very unusual in modern high-speed railway lines.

Aplicación del M.E.C. al estudio de sistemas elásticos con simetría axial

En este artículo se presenta la aplicación del Método de los Elementos de Contorno a la determinación del campo de desplazamientos y tensiones de sistemas axisimétricos en régimen elástico. Desarrollando asimismo, un procedimiento para la determinación de los coeficientes de las matrices de influencia que aparecen en el tratamiento numérico del problema. El estudio del estado tensional del sistema axisimétrico es de obvio interés en Ingeniería, pudiendo citarse entre otras las siguientes aplicaciones: estudio de vasijas de todo tipo, y cobrando plena actualidad las vasijas de los reactores nucleares; efecto de grietas y entallas; efecto de la colocación de zunchos de pretensado en depósitos de hormigon armado, etc. El tratamiento numérico de este tipo de problemas se produce como consecuencia de la dificultad de encontrar soluciones cerradas para las ecuaciones de campo que definen el problema, ecuaciones que aunque establecidas hace tiempo, sólo han sido resueltas en casos particulares. La ventaja de la utilización del M.E.C.,frente a los métodos de dominio, se pone de manifiesto en el estudio de este tipo de sistemas ya que la consideración de una malla monodimensional es suficiente para representar la discretización del contorno, produciendose una considerable reducción del tiempo de c��mputo.

Aplicación del M.E.C. a un problema de interacción suelo-estructura

Este artículo presenta la aplicación del M.E.C. a un problema de interacción suelo-estructura. Se trata de una estructura rígida empotrada a gran profundidad en un terreno muy duro y sometido a acciones sísmicas de importancia. Tras recordar los conceptos básico del problema se describe la discretización utilizada para la resolución mediante el método de los tres pasos. Se describe también la modificación inducida por la presencia de la estructura en la solicitación sísmica tanto en profundidad como en distancia a aquella.

Sampling strategies using the "accumulation chamber" for monitoring geological storage of CO2

Fundación Ciudad de la Energía (CIUDEN) is carrying out a project of geological storage of CO2, where CO2 injection tests are planned in saline aquifers at a depth of 1500 m for scientific objectives and project demonstration. Before any CO2 is stored, it is necessary to determine the baseline flux of CO2 in order to detect potential leakage during injection and post-injection monitoring. In November 2009 diffuse flux measurements of CO2 using an accumulation chamber were made in the area selected by CIUDEN for geological storage, located in Hontomin province of Burgos (Spain). This paper presents the tests carried out in order to establish the optimum sampling methodology and the geostatistical analyses performed to determine the range, with which future field campaigns will be planned.

Obtención del modelo tridimensional de la puerta de La Latina del S. XVI d.C. mediante equipo láser esc��ner terrestre.

El objetivo de este Proyecto Fin de Carrera (PFC) es la obtención de un modelo tridimensional de “La Puerta de la Latina”, ubicada en el aparcamiento delantero de la Escuela Técnica Superior de Arquitectura de la Universidad Politécnica de Madrid. El levantamiento se realiza con el equipo láser esc��ner terrestre Riegl LMS-Z420i. Tras la toma de datos se efectuará el tratamiento de la nube de puntos y se obtendrá una “imagen realista” del modelo, entendiendo por “imagen realista”una representación final en la que, partiendo del modelo digital triangulado, se realiza una asignación de texturas a partir de imágenes obtenidas in situ. Este proyecto pretende ser un ensayo de las posibilidades de esta tecnología en el proceso de la representación tridimensional de edificios de interés arquitectónico e histórico.