11 resultados para Cubic B-Spline

em Repositório Científico do Instituto Politécnico de Lisboa - Portugal


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A package of B-spline finite strip models is developed for the linear analysis of piezolaminated plates and shells. This package is associated to a global optimization technique in order to enhance the performance of these types of structures, subjected to various types of objective functions and/or constraints, with discrete and continuous design variables. The models considered are based on a higher-order displacement field and one can apply them to the static, free vibration and buckling analyses of laminated adaptive structures with arbitrary lay-ups, loading and boundary conditions. Genetic algorithms, with either binary or floating point encoding of design variables, were considered to find optimal locations of piezoelectric actuators as well as to determine the best voltages applied to them in order to obtain a desired structure shape. These models provide an overall economy of computing effort for static and vibration problems.

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Functionally graded materials are composite materials wherein the composition of the constituent phases can vary in a smooth continuous way with a gradation which is function of its spatial coordinates. This characteristic proves to be an important issue as it can minimize abrupt variations of the material properties which are usually responsible for localized high values of stresses, and simultaneously providing an effective thermal barrier in specific applications. In the present work, it is studied the static and free vibration behaviour of functionally graded sandwich plate type structures, using B-spline finite strip element models based on different shear deformation theories. The effective properties of functionally graded materials are estimated according to Mori-Tanaka homogenization scheme. These sandwich structures can also consider the existence of outer skins of piezoelectric materials, thus achieving them adaptive characteristics. The performance of the models, are illustrated through a set of test cases. (C) 2012 Elsevier Ltd. All rights reserved.

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A educação de crianças com necessidades educativas especiais (NEE) coloca nos nossos dias grandes desafios às escolas e famílias. A Inclusão apresenta-se neste contexto como a expressão chave, reveladora de um novo olhar e decidir, expressa na legislação, no discurso político e nas actuais disposições académicas e pedagógicas. Não obstante, nem todos os alunos com NEE dispõem de respostas integralmente inclusivas. Os alunos com espectro de Autismo, por exemplo, colocam às escolas e aos pais sérios problemas, os quais, devido à sua intensidade e variabilidade, questionam sem dúvida o sentido das respostas educativas adequadas a alunos portadores desta problemática. O objectivo geral deste estudo é, neste contexto, procurar aceder a um conhecimento mais actualizado sobre uma Unidade de Ensino Estruturado no atendimento a alunos com espectro de Autismo (UEEA). Pretende-se de modo mais específico aceder ao que pensam os professores sobre o atendimento educativo a alunos com espectro de Autismo e caracterizar uma unidade de ensino estruturado no que respeita aos recursos humanos, físicos e materiais, bem como as estratégias de trabalho privilegiadas no atendimento a este tipo de alunos e formas de colaboração entre técnicos e famílias. No sentido de melhor compreender e aprofundar esta problemática foram realizadas entrevistas semi-directivas a 3 professores do ensino especial com experiência em UEEA e a 3 professores do ensino regular. A escolha dos professores baseou-se em critérios relacionados com a sua experiência no atendimento a alunos com problemas de Autismo. A natureza do objecto de estudo induziu a um desenho de investigação de natureza interpretativa de carácter descritivo - Estudo de caso. O corpus do trabalho foi constituído pelas entrevistas semi-directivas, sujeitas a uma análise qualitativa de acordo com os procedimentos previsto para a análise de conteúdo. Com base na análise dos dados recolhidos, foi possível identificar e caracterizar aspectos relevantes sobre o que pensam os professores sobre a intervenção educativa de alunos com espectro de Autismo e sobre as respostas educativas existentes na UEEA.

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A imagem por difusão em RM caracteriza o movimento microscópico e aleatório das moléculas de água no tecido e a sua quantificação através do ADC permite avaliar a celularidade e estrutura do mesmo. O valor b corresponde ao factor de sensibilização à difusão, sendo que as imagens podem ser mais ou menos ponderadas em difusão. Segundo vários autores torna-se importante a determinação dos valores de b mais adequados pois este parâmetro é variável com o tipo de equipamento utilizado, podendo influenciar a qualidade diagnóstica do método.

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Mestrado em Medicina Nuclear.

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The phase diagram of a simple model with two patches of type A and ten patches of type B (2A10B) on the face centred cubic lattice has been calculated by simulations and theory. Assuming that there is no interaction between the B patches the behavior of the system can be described in terms of the ratio of the AB and AA interactions, r. Our results show that, similarly to what happens for related off-lattice and two-dimensional lattice models, the liquid-vapor phase equilibria exhibit reentrant behavior for some values of the interaction parameters. However, for the model studied here the liquid-vapor phase equilibria occur for values of r lower than 1/3, a threshold value which was previously thought to be universal for 2AnB models. In addition, the theory predicts that below r = 1/3 (and above a new condensation threshold which is < 1/3) the reentrant liquid-vapor equilibria are so extreme that it exhibits a closed loop with a lower critical point, a very unusual behavior in single-component systems. An order-disorder transition is also observed at higher densities than the liquid-vapor equilibria, which shows that the liquid-vapor reentrancy occurs in an equilibrium region of the phase diagram. These findings may have implications in the understanding of the condensation of dipolar hard spheres given the analogy between that system and the 2AnB models considered here. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4771591]

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Mestrado em Controlo e Gestão dos Negócios

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Relatório Final de Estágio apresentado à Escola Superior de Dança, com vista à obtenção do grau de Mestre em Ensino de Dança.

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We investigate the structural and thermodynamic properties of a model of particles with 2 patches of type A and 10 patches of type B. Particles are placed on the sites of a face centered cubic lattice with the patches oriented along the nearest neighbor directions. The competition between the self- assembly of chains, rings, and networks on the phase diagram is investigated by carrying out a systematic investigation of this class of models, using an extension ofWertheim's theory for associating fluids and Monte Carlo numerical simulations. We varied the ratio r epsilon(AB)/epsilon(AA) of the interaction between patches A and B, epsilon(AB), and between A patches, epsilon(AA) (epsilon(BB) is set to theta) as well as the relative position of the A patches, i.e., the angle. between the (lattice) directions of the A patches. We found that both r and theta (60 degrees, 90 degrees, or 120 degrees) have a profound effect on the phase diagram. In the empty fluid regime (r < 1/2) the phase diagram is reentrant with a closed miscibility loop. The region around the lower critical point exhibits unusual structural and thermodynamic behavior determined by the presence of relatively short rings. The agreement between the results of theory and simulation is excellent for theta = 120 degrees but deteriorates as. decreases, revealing the need for new theoretical approaches to describe the structure and thermodynamics of systems dominated by small rings. (C) 2014 AIP Publishing LLC.

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The phase diagram of a simple model with two patches of type A and ten patches of type B (2A10B) on the face centred cubic lattice has been calculated by simulations and theory. Assuming that there is no interaction between the B patches the behavior of the system can be described in terms of the ratio of the AB and AA interactions, r. Our results show that, similarly to what happens for related off-lattice and two-dimensional lattice models, the liquid-vapor phase equilibria exhibit reentrant behavior for some values of the interaction parameters. However, for the model studied here the liquid-vapor phase equilibria occur for values of r lower than 1/3, a threshold value which was previously thought to be universal for 2AnB models. In addition, the theory predicts that below r = 1/3 (and above a new condensation threshold which is < 1/3) the reentrant liquid-vapor equilibria are so extreme that it exhibits a closed loop with a lower critical point, a very unusual behavior in single-component systems. An order-disorder transition is also observed at higher densities than the liquid-vapor equilibria, which shows that the liquid-vapor reentrancy occurs in an equilibrium region of the phase diagram. These findings may have implications in the understanding of the condensation of dipolar hard spheres given the analogy between that system and the 2AnB models considered here.

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The associated production of a Higgs boson and a top-quark pair, t (t) over barH, in proton-proton collisions is addressed in this paper for a center of mass energy of 13 TeV at the LHC. Dileptonic final states of t (t) over barH events with two oppositely charged leptons and four jets from the decays t -> bW(+) -> bl(+)v(l), (t) over bar -> (b) over barW(-) -> (b) over barl(-)(v) over bar (l) and h -> b (b) over bar are used. Signal events, generated with MadGraph5_aMC@NLO, are fully reconstructed by applying a kinematic fit. New angular distributions of the decay products as well as angular asymmetries are explored in order to improve discrimination of t (t) over barH signal events over the dominant irreducible background contribution, t (t) over barb (b) over bar. Even after the full kinematic fit reconstruction of the events, the proposed angular distributions and asymmetries are still quite different in the t (t) over barH signal and the dominant background (t (t) over barb (b) over bar).