Orientador: Antonio de Queiroz Neto / Banca: José Corrêa de Lacerda Neto / Banca: Benedito Sérgio Denadai / Resumo: O esporte eqüestre vem exigindo um grau crescente de profissionalismo no mundo todo. Testes de desempenho, como a aferição do Limiar anaeróbio (LA), inserem-se neste contexto. Este trabalho comparou sete protocolos de mensuração do LA, cinco lactacidêmicos (V2, V4, LAI, LAI0,5, Lacmin) e dois glicêmicos (LGI e Glicmin). Todos foram comparados a Máxima fase estável do lactato (MFEL), protocolo padrão de aferição do LA. Catorze eqüinos Puro Sangue Árabe foram utilizados, entre machos e fêmeas. As médias e desvios-padrão das velocidades associadas aos testes foram: V2 = 9,49 ± 0,83 m/s, V4 = 10,83 ± 0,71 m/s, VLAI = 9,62 ± 0,91 m/s, VLAI0,5 = 10,21 ± 0,80 m/s, VLacmin = 7,49 ± 0,55 m/s, VLGI = 7,69 ± 1,68 m/s, VGlicmin = 8,31 ± 1,64 m/s e VMFEL = 6,06 ± 0,51 m/s. Somente a VLacmin não diferiu da VMFEL, além de obter correlação significativa com a mesma de ρ = 0,76 (Correlação de Spearman). A Tendência e os Limites de Concordância entre a VLacmin e a VMFEL foram de 1,43; 0,79 e 2,05. Além de predizer velocidades diferentes da VMFEL, os limiares LAI, LGI e Glicmin apresentaram dificuldades operacionais. As diferenças entre as velocidades preditas pelos protocolos V2, V4, LAI e LAI0,5, LGI e Glicmin a VMFEL podem ser parcialmente explicadas por variações de composição de protocolo e dificuldades operacionais. Apesar de não diferirem estatisticamente, as VLacmin e as VMFEL apresentaram baixa concordância, o que provavelmente pode ser melhorado com ajustes finos no protocolo do Lacmin. / Abstract: Equestrian sports are demanding a growing degree of professionalism all over the world. Performance tests, as Anaerobic threshold (AT) assessment, are inserted in that context. The present study compared seven protocols for anaerobic threshold assessment: five of them using the lactacidemia (V2, V4, IAT, IAT0.5 and Lacmin) and two glicemia (IGT and Glicmin). All of them were compared to the Maximal Lactate Steady State (MLSS), the gold standard for AT assessment. Fourteen Arabian horses, males and females were submitted to the protocols. Velocity means and standard deviation associated to each protocol were: V2 = 9.49 ± 0.83; V4 = 10.83 ± 0.71; VIAT = 9.62 ± 0.91; VIAT0,5 = 10.21 ± 0.80; VLacmin = 7.49 ± 0.55; VIGT = 7.69 ± 1.68; VGlicmin = 8.31 ± 1.64 e VMLSS = 6.06 ±0.51. Only VLacmin did not differ from VMLSS, moreover, they correlate significantly with ρ = 0.76 (Spearman correlation). Bias ant Limits of Agreement of the two methods were 1.43; 0.79 and 2.05. Besides they predicted different velocities when compared to VMLSS, IAT, IGT and Glicmin showed operational difficulties. The differences between the velocities associated with the several protocols and the VMLSS could be partially attributed to protocol components variations and some operational difficulties. Regardless the statistical equality, VLacmin and VMLSS revealed poor agreement, what could probably be improved with adjustments in the Lacmin protocol. / Mestre

A integridade da via auditiva e a investigação do respectivo limiar eletrofisiológico podem ser avaliadas por meio da observação, no domínio do tempo, dos potenciais evocados auditivos de tronco encefálico. Atualmente, nova técnica de análise dos potenciais evocados auditivos, no domínio das freqüências, tem sido utilizada para uma observação particular desses limiares. Assim, com a aplicação da transformada rápida de Fourier, é possível realizar a análise das freqüências comprometidas na audição, de maneira eficiente e rápida. O objetivo com este trabalho, então, foi desenvolver, caracterizar e realizar testes preliminares com um dispositivo único capaz de avaliar os potenciais evocados auditivos nos dois domínios, por meio de uma placa de som, que ainda não havia sido implementada para tal fim. Desse modo, foi produzido um aparelho capaz de registrar sinais biológicos da ordem de 0,5 ?V. Após a caracterização e o estudo simulado, foram conduzidos testes-piloto com doze seres humanos, ouvintes normais (n = 24 orelhas), divididos em dois grupos com o mesmo número de participantes. No grupo 1, os potenciais evocados auditivos de tronco encefálico adquiridos por meio de um instrumento padrão-ouro e de instrumento desenvolvido foram comparados entre si. Em seguida, os achados foram relacionados com o exame no domínio das freqüências formatado no novo aparelho. O grupo 2 foi submetido à avaliação dos potenciais miogênicos vestibulares, também com os dois instrumentos, e suas latências absolutas comparadas. Os resultados demonstraram não haver diferenças significativas entre os dois instrumentos para as amplitudes e latências do potencial evocado auditivo de tronco encefálico. Constatou-se, ainda, que as ondas presentes no domínio do tempo davam respostas equivalentes no domínio das freqüências. Por fim, também não foram encontradas diferenças significativas entre os dois aparelhos para as latências do potencial miogênico vestibular. / The integrity of the auditory pathway and the investigation of the respective electrophysiological threshold can be assessed by observation, in the time domain, of brainstem auditory evoked potentials. This assessment is usually evoked by clicks, which have a wide acoustic spectrum, and consequently serious limitations with respect to frequency specificity, in determining electrophysiological thresholds. New techniques for analyzing auditory evoked potentials in the frequency domain are currently being used for a closer observation of these thresholds. Thus, by applying the fast Fourier transform, one can analyzed the compromised auditory frequencies efficiently and rapidly. This method, on the other hand, does not investigate the integrity of specific auditory pathway structures, as the other method does. Although both types of assessment require similar biological amplifier architecture and are, to a certain extent, complementary, they are performed with two distinct devices. The first, which makes the observation in the time domain, is quite well known and several manufacturers have been producing it for a long time. The second, which inspects the potentials in the frequency domain, was introduced into the market only a few years ago. The aim of this study, therefore, was to develop, characterize and conduct preliminary tests with a single device capable of evaluating the auditory evoked potentials in both domains, by means of a sound card that had not been previously used for this purpose. Thus, a device was produced with biological amplifiers, filters, electrical protection apparatus and a logic control system capable of recording biological signals around 0.5 µV. After characterization and the simulated study, pilot tests were carried out with 12 normal- hearing subjects (n = 24 ears), allocated to two groups of 6 participants. In group 1, we observed the latencies and amplitudes of waves I, III and V of the brainstem auditory evoked potentials, using a gold standard instrument and a developed instrument and later compared them. The findings were then correlated to those of the frequency domain examination formatted on the new device. Group 2 was submitted to an assessment of components p13 and n23 of the vestibular myogenic potentials to observe the most delayed biological signals, also with both instruments, and their absolute latencies were compared. The results showed no significant differences between the two instruments for the amplitudes (p = 0.379; p = 0.301; p = 0.605, waves I, III and V, respectively) and latencies (p = 0.381; p = 0.140; p = 0.255) of the brainstem auditory evoked potentials. It was also found that the waves present in the time domain gave equivalent responses in the frequency domain. Finally, no significant differences were observed between the two devices for the absolute latencies of components p13 and n23 of the vestibular myogenic potentials, with p values of 0.102 and 0.078, respectively. Thus, it was concluded that the new instruments were efficient for the functions tested.

A compreensão dos caminhos de desativação não radiativa em polímeros conjugados é fundamental para o uso desses materiais em dispositivos luminescentes, células fotovoltaicas e sensores. Nesta tese, os processos não radiativos em filmes automontados de polímero luminescente foram investigados via análise da supressão de intensidade de fotoluminescência, utilizando a técnica de fluorescência estacionária, e através da medida do tempo de vida do estado excitado com fluorescência resolvida no tempo em arranjo de contagem de fótons. A camada emissiva constituída por poli(p-fenileno vinileno) (PPV) obtido da conversão térmica do precursor poli(cloreto de xilideno tetraidrotiofeno) (PTHT) apresentou tempos de vida entre 150 e 250 ps, e fraca dependência com o comprimento de onda de detecção da emissão. Na presença de uma monocamada contendo azocorante Vermelho do Congo (CR) ou ftalocianina tetrassulfonada de níquel (NiTsPc) atuando como receptor de energia foi observada supressão da fluorescência e encurtamento do tempo de vida (50-100ps). À medida que se aumenta a distância entre as camadas de doador e receptor via interposição de bicamadas de espaçador, a dinâmica do sistema tende à dinâmica de decaimento do estado excitado do PPV na ausência de receptor. A dependência da eficiência com a distância 1/r2 ou 1/r3 apontam para transferência de energia ressonante (RET) típica da interação plano-plano ou plano-camada. Os processos não radiativos foram também estudados em função da diluição de segmentos PPV dispersos em matriz de polieletrólito poli(cloreto de dodecildimetilamônio) PDAC. A diluição dos segmentos conjugados aumenta a eficiência quântica de emissão, torna o mecanismo de desativação mais lento (500 ps) e diminui a dependência do tempo de vida com o comprimento de onda de detecção, devido à menor eficiência dos mecanismos de desativação não radiativa. Na presença de uma camada receptora, a eficiência de transferência de energia é maior para amostras com segmentos mais diluídos indicando que esse mecanismo compete com os processos internos à própria camada emissiva. O tempo de vida aumenta em filmes com mais baixo grau de conjugação e a dependência com o comprimento de onda de emissão é mais forte. Em resumo, a técnica de automontagem se mostrou adequada para obter filmes com propriedades fotofísicas controláveis no nível molecular, que puderam ser estudadas com espectroscopias de fluorescência. / Understanding the pathway of excitation in conjugated polymers is important for using these materials as active layer in devices, photovoltaic cells and sensors. In this thesis, non-radiative processes in layer-by-layer (LbL) films were investigated with measurements of fluorescence quenching in steady-state fluorescence spectroscopy and of the singlet excited state lifetime using time-resolved fluorescence spectroscopy in a single photon counting (SPC) apparatus. The emissive layer of poly(p-phenylene vinylene) (PPV) obtained via thermal conversion of the soluble precursor poly(xylylidene tetrahydrothiophenium) chloride (PTHT) showed lifetime 150-250 ps and weak dependence on the emission wavelength. In the presence of an acceptor layer of either Congo Red (CR) or nickel tetrasulfonated phthalocyanine (NiTsPc) the PL intensity was quenched and the lifetime was shorter (50 -100 ps). Upon increasing the distance between the energy donor (PPV) and acceptor layers by interposing bilayers of inert polyelectrolytes the dynamics tended to the PPV dynamics. The distance-dependence of the energy transfer efficiency (1/r2 or 1/r3) points to a resonant process (RET) with a plane-to-plane or plane-to-slab interaction. The non-radiative processes were also studied for varying dilutions of the PPV segments in a matrix of the polyelectrolyte poly(dodecyl methylamonium chloride) (PDAC). This dilution increased the quantum efficiency and led to longer lifetimes (500 ps) owing to a less effective non-radiative energy transfer. When an energy acceptor layer is present, energy transfer is more efficient for the most diluted systems, indicating that such transfer competes with internal processes in the emissive layer. The lifetime increased in films with low degree of conjugation, for which there was a stronger dependence on the emission wavelength. It is concluded that the LbL methodology was suitable to obtain photophysical film properties that could be controlled at the molecular level, and investigated with varied fluorescence spectroscopies.

Com o objetivo de aumentar o lucro de plantas químicas, a Otimização em Tempo Real (RTO) é uma ferramenta que busca determinar as condições ótimas operacionais do processo em estado estacionário, respeitando as restrições operacionais estabelecidas. Neste trabalho foi realizada a implementação prática de um ciclo RTO em um processo de destilação por recompressão de vapor (VRD), propileno-propano, da Refinaria de Paulínia (Petrobras S.A.), a partir de dados históricos da planta. Foram consideradas as principais etapas de um ciclo clássico de RTO: identificação de estado estacionário, reconciliação de dados, estimação de parâmetros e otimização econômica. Essa unidade foi modelada, simulada e otimizada em EMSO (Environment for Modeling, Simulation and Optimization), um simulador de processos orientado a equações desenvolvido no Brasil. Foram analisados e comparados dois métodos de identificação de estado estacionário, um baseado no teste estatístico F e outro baseado em wavelets. Ambos os métodos tiveram resultados semelhantes e mostraram-se capazes de identificar os estados estacionários de forma satisfatória, embora seja necessário o ajuste de parâmetros na sua implementação. Foram identificados alguns pontos estacionários para serem submetidos ao ciclo RTO e foi possível verificar a importância de partir de um estado estacionário para a continuidade do ciclo, já que essa é uma premissa do método. A partir dos pontos analisados, os resultados deste estudo mostram que o RTO é capaz de aumentar o ganho econômico entre 2,5-24%, dependendo das condições iniciais consideradas, o que pode representar ganhos de até 18 milhões de dólares por ano. Além disso, para essa unidade, verificou-se que o compressor é um equipamento limitante no aumento de ganho econômico do processo. / In order to increase the profits of chemical plants, the Real-Time Optimization (RTO) is a tool that seeks to determine the steady-state optimal process operating conditions to maximize its profit under the operational restrictions. In this work, a practical implementation of a RTO cycle was implemented in a vapor recompression distillation (VRD) process, propylene-propane, from Paulínia Refinery (Petrobras S.A.), from historical plant data. The main steps of a classical RTO cycle are considered: steady-state identification, data reconciliation, parameter estimation and economical optimization. This unit was modeled, simulated and optimized in EMSO (Environment for Modeling, Simulation and Optimization), which is an equation oriented simulator conceived and developed in Brazil. Two steady state identification methods were analyzed and compared, one based on a F-like test and other based on wavelets. Both methods had similar results and showed to be able to identify the stationary states satisfactorily, although parameter tuning is necessary in their implementation. Some stationary points were identified and submitted to the RTO cycle. It was possible to verify the importance of start from a steady-state to continue the cycle, since this is a premise of the method. From the points analyzed, the results of this study show that the RTO is able to increase the economic gain between 2.5- 24%, depending on the initial conditions that is considered, which may represent gains of up to 18 million dollar per year. Furthermore, for this unit, it was found that the compressor is a limiting equipment in increasing economical gain.

Neste trabalho foi desenvolvido um estudo sobre a precessão livre de onda contínua (CWFP-continuous wave free precession), uma condição especial da precessão livre no estado estacionário (SSFP), e algumas aplicações. Os resultados experimentais, e de simulações, mostraram que este sinal é atingido após a passagem por dois estágios iniciais. O primeiro é dependente da não homogeneidade do campo magnético, relacionado a razão Tp/T2*. O segundo, o qual é chamado de estado quasi-estacionáio, é dependente ambos os tempos de relaxação do sistema em estudo, T1 e T2. Este segundo estágio é responsável por levar a magnetização do estado de equilíbrio térmico a um estado verdadeiramente estacionário. Tendo como informação a amplitude da magnetização no estado de equilíbrio térmico e no estado verdadeiramente estacionário, e também do decaimento do sinal durante o estado quasi-estacionário, é possível determinar, rápida e simultaneamente, ambos os tempos de relaxação do sistema, fazendo um único experimento. Esse método oferece aplicações interessantes para o estudo de processos dinâmicos, propostas também neste trabalho. Foi possível verificar que o sinal de CWFP pode ser utilizado para acompanhar cinética de reações, e também variações de viscosidade do meio, por exemplo, em reações de polimerização, associadas à mobilidade molecular em função de mudanças estruturais. Um método para avaliar a condutividade térmica de elastômeros foi proposto, com o fornecimento de resultados quantitativos muito próximos daqueles encontrados na literatura, e que utilizam outros métodos. A dependência do sinal de CWFP com a freqüência de offset também permitiu realizar um estudo, com aplicação em RMN de alta resolução, sobre a supressão de sinal de solvente. Os resultados demonstraram que é necessário fazer alguns ajustes na largura de pulsos, juntamente com o ciclo de fases, para minimizar as anomalias de intensidade e de fase dos sinais no espectro transformado. Essa técnica foi aplicada em espectroscopia ‘in vivo’, a qual permite resolver, por exemplo, problemas como a determinação de açúcares em frutas, onde o sinal é bastante próximo do intenso sinal da água. / In this work a study of the continuous wave free precession (CWFP), a special condition of the steady-state free precession (SSFP), and some applications, was developed. The experimental results, together with simulated ones, have shown that the CWFP signal is attained after two previous stages. The first one is dependent on the non-homogeneity of the magnetic field, related to Tp/T2* ratio. The second, which is called quasi-stationary state, is dependent of both relaxation times, T1 and T2. This second stage allows leading the magnetization in the thermal equilibrium to a truly stationary state. The information of the signal amplitude in the thermal equilibrium and in the steady state, and also the signal decaying during the quasistationary state, allows the fast and simultaneous determination of the relaxation times, performed in a single experiment. This method offers interesting applications for studying dynamical processes, also proposed in this work. It was possible to verify that the CWFP signal can be used to monitor kinetics of reactions, which variations of viscosity are involved, for example, in polymerization reactions, always associated to structural changes. A method for evaluating thermal conductivity in elastomers was proposed, with results in accordance to the literature, which uses other methods. The dependence of the CWFP signal with the offset frequency has permitted to study an application to the High-Resolution NMR, about the solvent suppression. The results demonstrated that it is necessary to perform some adjustments in the pulse width, together the phase cycle, to minimize some phase and intensity anomalies of the frequency-domain signal. This technique was applied in ‘in vivo’ spectroscopy, which can solve, for example, problems with the determination of the sugar content in fresh fruits, where the sugar signal is very close to the intense signal of the water.

Este estudo reúne os principais resultados de fluorescência estática e resolvida no tempo sobre a interação da porfirina meso-tetrakis (4-metilpiridil), na forma de base livre (TMPyP) e complexada com Zn2+ (ZnTMPyP), com vesículas de fosfolipídio. Adicionalmente foram utilizadas as técnicas de potencial zeta e espalhamento de luz dinâmico (DLS, do inglês \"dynamic light scattering\"). As vesículas de fosfolipídio foram formadas por dois conjuntos de fosfolipídios: saturados e insaturados. O primeiro grupo é formado pela mistura dos fosfolipídios zwiteriônico 1,2-dipalmitoil-sn-glicero-3-fosfocolina (DPPC) e aniônico 1,2-dipalmitoil-sn-3-glicero-[fosfo-rac-(1- glicerol)] (DPPG), a diferentes razões molares. Os estudos utilizando tais sistemas foram realizados abaixo (25oC) e acima (50oC) da temperatura de transição de fase gel-líquido cristalino destes fosfolipídios (~ 41oC). O segundo grupo é formado pela mistura dos fosfolipídios zwiteriônico 1-palmitoil-2-oleoil-sn-glicero-3-fosfocolina (POPC) e aniônico 1-palmitoil-2-oleoil-sn-glicero-3-fosfo(1-rac-glicerol) (POPG). Como a transição de fase destes dois fosfolipídios ocorre a temperaturas negativas, todos os experimentos foram realizados a 25oC (vesículas no estado líquido cristalino). Todos os sistemas foram preparados através do método de extrusão para a obtenção de vesículas grandes unilamelares (LUV, do inglês \"large unilamellar vesicles\"). As análises dos dados de fluorescência indicaram que a atração eletrostática entre os substituíntes (positivamente carregados) das porfirinas TMPyP e ZnTMPyP e o grupo das cabeças polares (camada de Stern) das vesículas de fosfolipídio desempenha um papel fundamental na associação da porfirina. A distribuição da TMPyP entre o meio aquoso (tampão) e as vesículas de fosfolipídio foi evidenciada pela coexistência de um tempo de vida de fluorescência mais curto (~ 5 ns) e outro mais longo (~ 9-11 ns), respectivamente. Baseado nos valores das constantes pré-exponenciais, estudos adicionais mostram que a distribuição acima é afetada pela concentração de sal na solução. Os resultados de supressão de fluorescência com o supressor iodeto de potássio (KI) indicaram que ambas porfirinas estão localizadas, preferencialmente, na região da camada de Stern. Este resultado foi confirmado pelos estudos de potencial zeta e de DLS, os quais mostraram uma neutralização parcial das cargas negativas na superfície das vesículas devido à associação da porfirina. / This study presents time-resolved and steady-state fluorescence results on the interaction of the meso-tetrakis (4-methylpyridil) porphyrin, in free base form (TMPyP), and complexed with Zn2+ (ZnTMPyP), with phospholipid vesicles. Zeta potential and dynamic light scattering (DLS) techniques were also used. Phospholipid vesicles were formed by two phospholipid systems: saturated and unsaturated. The first group is a mixture of zwiterionic dipalmitoyl-sn-glycero-3-phosphocoline (DPPC) and anionic 1,2-dipalmitoyl-sn-3-glycero-[phospho-rac-(1-glycerol)] (DPPG) phospholipids, at different molar ratios. Measurements were performed bellow (25oC) and above (50oC) the main gel-liquid crystalline phase transition temperature (~ 41oC). The second group is constituted by a mixture of zwiterionic 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocoline (POPC) and anionic 1-palmitoyl-2-oleoyl-sn-glycero-3-phospho(1-rac-glycerol) (POPG) phospholipids, at different molar ratios. Since the gel-liquid crystalline phase transition of these phospholipids occurs at a very low temperature value, all experiments were performed at 25oC (liquid crystalline state vesicles). All phospholipid systems were prepared through the extrusion method in order to obtain large unilamellar vesicles (LUV). The fluorescence data analyses indicated that the electrostatic attraction between the porphyrin substituents (positively charged) and the polar head groups of the phospholipid vesicles (Stern layer) plays an important role on the porphyrin binding affinity. The distribution of TMPyP between the aqueous medium (buffer) and the phospholipid vesicles was characterized by the coexistence of a shorter (~ 5 ns) and a longer (~ 9-11 ns) fluorescence lifetimes, respectively. Based on the pre- exponential values, additional time-resolved experiments showed a redistribution of the porphyrin at increasing salt concentration. The quenching studies, using potassium iodide (KI) as quencher, indicated that both TMPyP and ZnTMPyP are preferentially located at the Stern layer region. This result is in agreement with the zeta potential and DLS findings, which demonstrated a partial neutralization of the negative charges at the vesicle surface due to the porphyrin association.

L’Imagerie par Résonance Magnétique (IRM) est une belle application de la physique et constitue sans aucun doute l’une des techniques les plus performantes d’imagerie médicale. Basée sur le phénomène de la Résonance Magnétique Nucléaire (RMN) du proton contenu dans les molécules d’eau, l’IRM permet d’investiguer en coupes les tissus mous du corps, sur base de contrastes différents. La méthode est non-invasive et n’utilise pas de radiations ionisantes. En plus des données morphologiques, l’IRM permet également d’obtenir des informations fonctionnelles et physiologiques.<p>De nos jours, plus de 10 000 unités IRM existent dans le monde et des millions d’examens sont réalisés chaque année. La technique est en constant développement et le domaine de recherches est multidisciplinaire. Il concerne aussi bien les développements méthodologiques (imagerie rapide, imagerie de diffusion, etc.) que technologiques (imagerie à haut champ, systèmes de gradients à commutation rapide, etc.), le point central des recherches étant l’amélioration de la qualité des images et la diminution du temps d’acquisition. Ceci implique l'optimisation des différentes séquences IRM (séries d'impulsions radiofréquence et de gradients de champ magnétique) tenant compte des contraintes imposées par le matériel, ainsi que le développement et l'optimisation du matériel lui-même. Cette thèse est consacrée au design avancé des séquences d’impulsions et contribue donc à l'optimisation des schémas d’acquisition en IRM.<p>En particulier, le présent travail est focalisé sur la compréhension et l’amélioration d’un certain type de séquences rapides, employant des échos de gradients :les séquences Steady-State Free Precession (SSFP) et plus précisément les séquences dites balanced-SSFP. Dans ce genre de schéma d’acquisition, le système est excité rapidement et périodiquement, conduisant à l’établissement d’un état stationnaire de l’aimantation. <p>La première partie de la thèse est consacrée à une analyse approfondie des propriétés du signal dans une séquence balanced-SSFP, à la fois à l’état stationnaire et à l’état transitoire. Ensuite, de nouveaux schémas d’acquisition sont développés sur base de calculs analytiques et de simulations numériques et sont ensuite testés expérimentalement. D’une part, une manipulation de l’état stationnaire est présentée en vue de supprimer le signal de la graisse sur les images (qui peut être gênant pour le diagnostic de certaines lésions ou maladies). D’autre part, l’application d’une phase de préparation en vue d’obtenir un contraste basé sur le degré de diffusion des molécules d’eau dans les tissus est analysée en détails, afin d’améliorer la qualité d’image produite par des séquences de diffusion existantes.<p>La présente thèse constitue donc un travail de recherches théoriques et expérimentales, allant de la conception de nouveaux schémas d’acquisition à leur expérimentation sur volontaires, en passant par leur implémentation sur un imageur IRM. Ce travail a été réalisé au sein de l’Unité d’IRM – Radiologie de l’Hôpital Erasme, sous la direction de Thierry Metens, Docteur en Sciences et Physicien IRM.<p> / Doctorat en Sciences / info:eu-repo/semantics/nonPublished

Preliminary studies have stirred the hope that sound-field stimulation through auditory steady state evoked potentials can be used to assess aided thresholds in the difficult-to-test population. Before the introduction of ASSEP into the clinical field, as a technique for the prediction of aided thresholds in the difficult-to-test population, a question arises concerning its clinical validation. The application of ASSEP through sound field stimulation, in the determination of aided thresholds and for the evaluation of amplification fittings, is dependent on the determination of unaided responses. Subsequently the estimation of unaided thresholds in the hearing impaired population is dependent on the establishment of normative data from the normal hearing population. The aim of this study was to determine the influence of insert earphones and sound field speaker presentation on threshold estimations using monotic auditory steady state evoked potentials, in a group of normal hearing adults. To achieve the aim of the study, a comparative, within-group experimental design was selected. The results of the current study indicated that the monotic single ASSEP technique under both insert earphone- and sound field conditions provided a reasonable estimation (25-35 dB HL for inset earphones; 20-33 dB HL for sound field speaker presentation) of the behavioural pure tone thresholds. The minimum response levels obtained under insert earphone conditions differed significantly from those obtained under sound field conditions for all the frequencies tested except 2 kHz (p < 0.01). Subsequently, the current study indicates that minimum response levels obtained using a specific transducer should serve as the basis of comparison with behavioural thresholds obtained under the same transducer. Therefore, behavioural pure tone thresholds obtained under insert earphone conditions will not suffice as a basis of comparison for minimum response levels obtained for the ASSEP technique under sound field conditions, and vice versa. This research endeavour concluded that the monotic ASSEP technique under both insert earphone and sound field conditions provide useful information for the estimation of frequency specific thresholds, but that the results are transducer specific and that comparison across transducers should be avoided. / Dissertation (M (Communication Pathology))--University of Pretoria, 2006. / Speech-Language Pathology and Audiology / Unrestricted

Cette recherche s’articule en deux parties. L’objectif de la première partie est d’analyser par voie expérimentale et numérique la phénoménologie du décollement interne, dit décollement de jet (en regimes transitoire et établi) dans les tuyères supersoniques refroidies par film fluide. La deuxième partie porte sur la réinterprétation des concepts de tuyère existants pour aboutir à la proposition d’un nouveau dispositif de détente supersonique, qui offre une résistance accrue au décollement de jet. La première partie de cette thèse est basée sur l’analyse des résultats expérimentaux obtenus lors de la campagne d’essais réalisée à l’ONERA. Ces essais, ont mis en évidence des spécificités de comportement de la tuyère, inhérentes à la manière d’amorcer le jet supersonique principal par rapport à l’établissement du film pariétal. Ces mêmes expériences ont permis d’étudier le comportement instationnaire du décollement de jet lorsque les conditions d’alimentation sont maintenues en régime établi. L’apparition de fréquences caractéristiques a été mise en évidence et leur origine a été étudiée à l’aide de simulations numériques. En nous appuyant sur les considérations issues de la première partie de l’étude, une revue critique des concepts de tuyère existants a été menée. Ce travail a permis d’identifier une lacune majeure dans la définition des tuyères à écoulement interne, à savoir l’absence d’une « barrière » qui puisse prévenir l’occurrence du décollement de jet. Ainsi, nous avons proposé la conjonction d’un dispositif à écoulement externe (aerospike) et d’une tuyère classique afin de résoudre cette problématique in nuce, en créant une barrière fluidique continue tout autour du plan de sortie de la tuyère principale. L’efficacité de ce concept a donc été prouvée par calcul, puis une campagne expérimentale a été organisée afin de valider les résultats obtenus. / This research is in two parts. The objective of the first part is to analyse by experimental and numerical means the phenomenology of nozzle flow separation in transient and steady state conditions. The second part of this research work focuses on the reinterpretation of existing concepts of converging-diverging nozzles, leading to the proposal of a new supersonic expansion device, with improved flow separation characteristics.Experimental data, collected during the test campaign conducted at ONERA, have been analysed and are presented in the first part of this thesis. Obtained results highlight some peculiarities of the transient behavior of the nozzle, mostly dependent on the synchronisation between the start-up phase of the main jet and the grow-up of the wall film. These same experiments have been also used to investigate the unsteadiness of the flow separation, when nozzle feeding conditions are maintained constant. Appearance of characteristic frequencies has been highlighted and their origin has been investigated by CFD simulations.In the second part, a critical review of existing nozzle concepts was conducted. This allowed identifying a major gap in the definition of traditional supersonic nozzles, namely the absence of a "barrier" that can prevent the occurrence of the flow separation. Thus, in the second part of this thesis we propose a new nozzle concept. It is based on the combination of a small aerospike and a conventional nozzle (main flow). Such an arrangement allows solving the flow separation problem in nuce. The effectiveness of this concept has been proved by calculation and by an experimental test campaign.

La croissance cristalline de KH2PO4(KDP)and K(H1-xDx)2PO4(DKDP)a été fortement étudiée depuis de nombreuses années. Les propriétés optiques nonlinéaires (conversion de fréquence: doublage pour le KDP et triplage pour le DKDP)et les études fondamentales sur les mécanismes de croissance sont à la base du développement important de la croissance de ces cristaux. Au début des années 90, un fort intérêt s'est porté sur le KDP et DKDP pour les dispositifs optiques à large ouverture pour les applications industrielles de fusion inertielle comme au NAtional Ignition Facility (NIF) aux USA ou pour le laser MégaJoule en France. La dimension de ces optiques (40*40 cm²) nécessite des cristaux géants crûs en solution. Une technique de croissance rapide a été développé par abaissement de température dans un réacteur de 1000L et par une filtration en continu afin d'éviter la nucléation spontanée. Cette méthode est très robuste et fiable pour la croissance rapide de cristaux géants de KDP mais néanmoins montre des limitations inhérentes à cette méthode. En effet, cela mène à des cristaux inhomogènes (défauts, inhomogénéités isotopiques)ce qui est rédhibitoire pour des solutions solides intermédiaires comme le DKDP : la composition en début de croissance peut varier significativement de celle en fin de croissance. Très récemment, des méthodes par circulation de solution en conditions stationnaires ont été développées pour palier à ce problèmeet sont considérées comme les plus pertinentes. C'est pourquoi nous avons développé un système par circulation en conditions stationnaires avec un traitement original de la solution. Dans un premier temps, le système a été testé sur un composé modèle KDP puis dans un deuxième sur le composé utilisé pour l'application DKDP. / Crystal Growth of KH2PO4(KDP)and K(H1-xDx)2PO4(DKDP)has been extensively covered over the years. For decades KDP and DKDP crystals have been grown either for their nonlinear optical properties (frequency conversion : doubling for KDP and tripling for DKDP) or for fundamental studies on crystal growth mechanisms. At the beginning of the 90's, a special interest arose for KDP for large aperture optical elements for laser fusion facilities such as the National Ignition Facility (NIF)in the USA or for the laser MegaJoule in France. The size of such optics(40*40 cm²)requires giant crystals to be grown in solution. A rapid growth technique has been developed based on the temperature lowering of a 1000L solution and its continuous filtration to avoid spurious nucleation. While this method is very robust and fully mature for the rapid growth of giant KDPs it nonetheless suffers from the limitations inherent to the Temperature Lowering Method(TLM).It does not provide stable growth conditions(temperature and supersaturation change).This can lead to inhomogeneous crystals (defects, isotopic inhomogeneity)and this is critical for intermediate of a solid solutions as the DKDP : the composition grown at the beginning can differ significantly from the one crystallizing later. Very early, transport methods growing crystals in stationary conditions, were considered to be "the most pertinent ones". That's why we have developed a growth system in stationary conditions with an original treatment of the solution. The grown compound selected was firstly KDP (model compound)then DKDP (KDP deuterated) for the desired application.