4 resultados para Planar array
Resumo:
Presented at Faculdade de Ciências e Tecnologias, Universidade de Lisboa, to obtain the Master Degree in Conservation and Restoration of Textiles
Resumo:
Application of Experimental Design techniques has proven to be essential in various research fields, due to its statistical capability of processing the effect of interactions among independent variables, known as factors, in a system’s response. Advantages of this methodology can be summarized in more resource and time efficient experimentations while providing more accurate results. This research emphasizes the quantification of 4 antioxidants extraction, at two different concentration, prepared according to an experimental procedure and measured by a Photodiode Array Detector. Experimental planning was made following a Central Composite Design, which is a type of DoE that allows to consider the quadratic component in Response Surfaces, a component that includes pure curvature studies on the model produced. This work was executed with the intention of analyzing responses, peak areas obtained from chromatograms plotted by the Detector’s system, and comprehending if the factors considered – acquired from an extensive literary review – produced the expected effect in response. Completion of this work will allow to take conclusions regarding what factors should be considered for the optimization studies of antioxidants extraction in a Oca (Oxalis tuberosa) matrix.
Resumo:
This present study aimed to investigate the fatigue life of unused (new) endodontic instruments made of NiTi with control memory by Coltene™ and subjected to the multi curvature of a mandibular first molar root canal. Additionally, the instrument‟s structural behaviour was analysed through non-linear finite element analysis (FEA). The fatigue life of twelve Hyflex™ CM files was assessed while were forced to adopt a stance with multiple radius of curvature, similar to the ones usually found in a mandibular first molar root canal; nine of them were subjected to Pecking motion, a relative movement of axial type. To achieve this, it was designed an experimental setup with the aim of timing the instruments until fracture while worked inside a stainless steel mandibular first molar model with relative axial motion to simulate the pecking motion. Additionally, the model‟s root canal multi-curvature was confirmed by radiography. The non-linear finite element analysis was conducted using the computer aided design software package SolidWorks™ Simulation, in order to define the imposed displacement required by the FEA, it was necessary to model an endodontic instrument with simplified geometry using SolidWorks™ and subsequently analyse the geometry of the root canal CAD model. The experimental results shown that the instruments subjected to pecking motion displayed higher fatigue life values and higher lengths of fractured tips than those with only rotational relative movement. The finite element non-linear analyses shown, for identical conditions, maximum values for the first principal stress lower than the yield strength of the material and those were located in similar positions to the instrument‟s fracture location determined by the experimental testing results.
Resumo:
Estudamos teoricamente as transi ções de Fr éedericksz nas geometrias interm édias entre: (i) afunilamento e tor ção (ii) tor ção e flexão; e (iii) fexão e afunilamento. Foram determinadas as condi ções em que a transi ção entre o estado não deformado e o estado homogeneamente deformado (transi ção de Fr éedericksz usual) e substituída pela transi ção entre o estado não deformado e o estado deformado com estrutura peri ódica. Tamb ém estudamos te órica e experimentalmente a dinâmica de reorienta ção do campo do director ap os rota ção s ubita da amostra num campo magn ético uniforme. Consideramos monodomí nios de cristais l íquidos nem áticos uniaxiais não quirais diamagnéticos de baixo peso molecular, contidos entre duas fronteiras planas uniformes paralelas e r ígidas com alinhamento planar. Simulamos e reproduzimos, na geometria de tor ção toda a evolu ção do campo do director desde o momento em que se impõe uma rota ção s úbita e at é ao instante em que se observa a forma ção de bandas.