Orientador: Gustavo Silva Wiederhecker / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin / Made available in DSpace on 2018-09-02T10:33:51Z (GMT). No. of bitstreams: 1 Luiz_GustavoDeOliveira_D.pdf: 5507367 bytes, checksum: 506db63a5a93a33d67a84dbb1f7b33ce (MD5) Previous issue date: 2017 / Resumo: Nas últimas décadas a optomecânica de microcavidades chamou a atenção de cientistas e engenheiros, que encontraram na interação entre luz e ondas acústicas aplicações que variam de sensores de massa com resolução atômica, até a preparação de estados quânticos de osciladores harmônicos mesoscópicos, passando por simuladores quânticos, filtros ópticos controláveis opticamente, criação de estados topológicos para luz e fônons, apenas citando alguns exemplos. Apesar das diversas demonstrações de vários dispositivos, sendo discos e cristais fotônicos os formatos mais comuns, há ainda um grande esforço no sentido de aperfeiçoá-los reduzindo perdas ópticas e mecânicas e suprimindo outros fenômenos de óptica não-linear, como absorção de dois fótons, que podem impedir seu funcionamento apropriado. Como ressonadores ópticos e mecânicos tipicamente compartilham a mesma estrutura nestes dispositivos, seus projetos são acoplados, dificultando o aprimoramento independente de cada um. Nesta tese usamos dispositivos optomecânicos de campo próximo, cuja interação entre modos mecânicos e ópticos se dá através do campo evanescente do último, para desacoplar o projeto mecânico do óptico, o que nos permitiu estudar a otimização do ressonador mecânico sem qualquer efeito sobre a cavidade óptica. Com um ressonador mecânico de silício composto por dois osciladores acoplados, pudemos demonstrar que o correto equilíbrio das massas de cada oscilador é um método simples e eficiente para suprimir as perdas devido à radiação de energia mecânica para o substrato na escala de frequência de 50 MHz. Este processo permitiu que fatores de qualidade limitados por perdas relacionadas ao material e à superfície, da ordem de 10 mil à temperatura ambiente e de 50 mil a aproximadamente 25 K, fossem obtidos. Também observamos nestes dispositivos o fenômeno de auto-pulsação, que apresenta uma dinâmica própria tão interessante quanto a optomecânica, apesar de impedir a operação apropriada dos osciladores optomecânicos. Estudamos este fenômeno separadamente e demonstramos que estes pulsos, ocorrendo em duas cavidades ópticas acopladas por seus campos evanescentes, podem sincronizar com o campo óptico sendo o único intermediador. Ambas as demonstrações têm implicações importantes, abrindo caminho para o desenvolvimento de novas plataformas de interesse tanto científico quanto tecnológico, como estruturas para o estudo de estados topológicos para a luz e para ondas acústicas e geradores de sinal de radio-frequência de alto desempenho. Além disso, os dispositivos foram todos produzidos em uma fábrica comercial, o que também demonstra que sua fabricação está pronta para ser escalada para produção em massa / Abstract: Cavity optomechanics in the micro-scale has attracted the attention of scientists and engineers on the last few decades, who encountered applications to the interaction of light and acoustic waves ranging from atomic resolution mass sensors to the preparation of quantum states of mesoscopic harmonic oscillators, passing by quantum simulators, optically controllable optical filters, formation of topological states for both photons and phonons, just to mention a few examples. Although various devices have been demonstrated, with disks and photonics crystals being the most common designs, there is still a large effort to improve them by reducing optical and mechanical losses and suppressing other non-linear phenomena, such as two-photon absorption, that may affect their proper operation. Because optical and mechanical resonators typically share the same structure in these devices, their designs are coupled, which complicates the independent improvement of each one. In this thesis we used near-field optomechanical devices, whose mechanical modes interact with the optical through the latter¿s evanescent field, to decouple the mechanical design from the optical, what allowed us to focus all attention on the mechanical resonator. With a silicon mechanical resonator composed of two coupled oscillators, we could demonstrate that the correct balance of the masses of the oscillators is an efficient and simple way to suppress losses due to energy radiation to the substrate at the 50 MHz frequency range. This strategy led to material and surface limited quality factors close to 10k at room temperature and 50k at approximately 25 K. We also observed the phenomenon of self-pulsing in these devices, which presents dynamics as interesting as the optomechanical interactions do, in spite of being a problem for the proper operation of the optomechanical devices. We studied this phenomenon separately and demonstrated that these pulses, when occurring in two evanescently coupled optical cavities, may synchronize with the optical field being the sole intermediary. These two demonstrations have important implications, paving the way for new platforms of scientific and technological interest, such as structures for the study of topological states for both light and acoustic weaves as well as high efficiency radio-frequency signal generators. Moreover, these devices were all fabricated in a commercial foundry, which also demonstrates that the fabrication of such technology is ready to be scaled up to mass production / Doutorado / Física / Doutor em Ciências / 153044/2013-6 / CNPQ

We try to explain the mathematical theory of thin liquid film evolution. We start with introducing physical processes in which thin film evolution plays an important role. Derivation of the classical thin film equation and existing mathematical theory in the literature are also introduced. To explain the thin film evolution we derive a new family of degenerate parabolic equations. We prove results on existence, uniqueness, long time behavior, regularity and support properties of solutions for this equation. At the end of the thesis we consider the classical thin film Cauchy problem on the whole real line for which we use asymptotic equipartition to show H^1(R) convergence of solutions to the unique self-similar solution.

The load-carrying and energy-dissipation capacities of ultra-high-performance concrete (UHPC) under dynamic loading are evaluated in relation to microstructure composition at strain rates on the order of 10⁵ s⁻¹ and pressures of up to 10 GPa. Analysis focuses on deformation and failure mechanisms at the mesostructural level. A cohesive finite element framework that allows explicit account of constituent phases, interfaces, and fracture is used. The model resolves essential deformation and failure mechanisms in addition to providing a phenomenological account of the effects of the phase transformation. Four modes of energy dissipation are tracked, including pressure-sensitive inelastic deformation, damage through the development of distributed cracks, interfacial friction, and energy released through phase transformation of the quartz silica constituent. Simulations are carried out over a range of volume fractions of constituent phases to quantify trends that can be used to design materials for more damage-resistant structures. Calculations show that the volume fractions of the constituents have more influence on the energy-dissipation capacity than on the load-carrying capacity, that inelastic deformation is the source of over 70% of the energy dissipation, and that the presence of porosity changes the role of fibers in the dissipation process. The results also show that the phase transformation has a significant effect on the load-carrying and energy-dissipation capacities of UHPC for the conditions studied. Although transformation accounts for less than 2% of the total energy dissipation, the phase transformation leads to a twofold increase in the crack density and yields nearly an 18% increase to the overall energy dissipation. Microstructure-behavior relations are established to facilitate materials design and tailoring for target-specific applications.

Recently, powders of the size d (0.1 μm < d < 10 μm) have been referred to ultrafine particles. The particle shape considered is assumed to be a sphere of the diameter d. The handling of powders is of great importance for processing of pharmaceuticals, cement, chemicals and other products. Most of these technological processes involve powder compaction, storage, transportation, mixing, etc, therefore, understanding of the fundamentals of particles interaction behaviour is very essential in the design of machines and equipment as well as in powder technology, cleaning of environment and other areas. The dynamic behaviour of particulate systems is very complicated due to the complex interactions between individual particles and their interaction with the surroundings. Understanding the underlying mechanisms can be effectively achieved via particle scale research. The problem of a normal contact may be resolved in a number of ways. In spite of huge progress in experimental techniques, direct lab tests with individual particles are still rather time-consuming and expensive. The interaction of particles as solid bodies is actually a classical problem of contact mechanics. In the case of ultrafine particles, the reduction of the particle size shifts the contact zones into the nanoscale or subnanoscale. Thus, steadily increasing contribution of adhesion has to be considered in the development of the physically correct constitutive models and numerical tools. Consequently, it may... [to full text] / Ultrasmulkios dalelės yra šiuolaikinės chemijos, farmacijos, maisto ir kitų pramonės šakų produktų sudėtinė dalis. Tiriant pramoninius technologinius procesus, neišvengiamai reikalingos teorinės žinios apie ultrasmulkių dalelių elgseną. Išsamus supratimas įmanomas tik atlikus įvairius tyrimus. Pastaruoju metu milteliai, klasifikuojami kaip ultrasmulkios (0,1 < d < 10 μm) dalelės, imti plačiai naudoti pramoniniuose procesuose, todėl suprasti ultrasmulkių dalelių elgsenos fundamentalumą miltelių technologijoje yra labai svarbu. Ultrasmulki dalelė yra itin maža, todėl su ja atlikti fizinį eksperimentą, kuris reikalauja specialios įrangos bei žinių, labai sunku. Tokiu atveju dažniausiai naudojamas skaitinis eksperimentas, kurį galima atlikti virtualiai. Skaitinio eksperimento metu yra tiriamos dinaminės ultrasmulkios dalelės savybės bei sprendžiamas dinaminis uždavinys. Taikant skaitinius modelius bei dalelės judėjimą aprašančias jėgų lygtis, naudojami sąveikos modeliai, apimantys adhezinę, klampią, tamprią bei tampriai plastinę sąveikas. Mikroskopinis adhezinės sąveikos modeliavimas – aktualus mechanikos mokslo uždavinys. Taikant sąveikos modelius, svarbu pritaikyti ir diskrečiųjų elementų metodą, kadangi, norint aprašyti dalelių elgseną, visų pirma reikia su-vokti ir aprašyti dalelės modelį. Dalelės elgsenos skaitiniam modeliavimui siūlomi teoriniai modeliai leidžia tirti dalelės sąveiką su dalele ar tampria puserdve bei sąveikos dinamiką. Šie modeliai galėtų būti pritaikyti... [toliau žr. visą tekstą]

The ability to adjust structural response to external loading and ensure structural safety and serviceability is a characteristic of Smart Systems. The key to achieving this is through the development and implementation of smart materials. An example of a smart material is a Shape Memory Alloy (SMA). Reinforced concrete structures are designed to sustain severe damage and permanent displacement during strong earthquakes, while maintaining their integrity, and safeguarding against loss of life. The design philosophy of dissipating the energy of major earthquakes leads to significant strains in the steel reinforcement and, consequently, damage in the plastic hinge zones. Most of the steel strain is permanent, thus leading to large residual deformations that can render the structure unserviceable after the earthquake. Alternative reinforcing materials such as superelastic SMAs offer strain recovery upon unloading, which may result in improved post-earthquake recovery. Shape Memory Alloys have the ability to dissipate energy through repeated cycling without significant degradation or permanent deformation. Superelastic SMAs possess stable hysteretic behavior over a certain range of temperature, where its shape is recoverable upon removal of load. Alternatively, Martensite SMAs also possess the ability to recover its shape through heating. Both types of SMA demonstrate promise in civil infrastructure applications, specifically in seismic-resistant design and retrofit of structures. The primary objective of this research is to investigate experimentally the performance of concrete beams and shear walls reinforced with superelastic SMAs in plastic hinge regions. Furthermore, this research program involves complementary numerical studies and the development of a proposed hysteretic constitutive model for superelastic SMAs applicable for nonlinear finite element analysis. The model considers the unique characteristics of the cyclic response of superelastic materials.

Made available in DSpace on 2014-06-11T19:23:39Z (GMT). No. of bitstreams: 0 Previous issue date: 2009-12-11Bitstream added on 2014-06-13T20:50:43Z : No. of bitstreams: 1 morais_vs_me_ilha.pdf: 9848157 bytes, checksum: 187eadcaad3e9775d2aa107935283406 (MD5) / Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) / Este trabalho dá continuidade e aperfeiçoa um modelo automatizado para estimativa de altura de ondas geradas em lagos de barragens, a partir dos dados característicos de vento. Infere sobre a climatologia dos ventos, a fim de determinar as maiores alturas de ondas e identificar pontos críticos, tanto para a segurança à navegação, quanto para as margens do reservatório. Lagos de barragens, foco desta dissertação são, em sua maioria, dotados de vegetação aquática. Dentro dessa temática, uma busca por modelos capazes de qualificar e quantificar o quão as ondas geradas pelo vento reagem ao atravessar esses obstáculos naturais em termos de oscilação das plantas, presentes nas margens, foi também discutida. Para os propósitos aqui expostos, um aplicativo computacional foi utilizado para a previsão de ondas e estruturado de maneira que pudesse fornecer resultados gráficos de forma automatizada com maior precisão e no menor tempo possível. O software, fruto do desenvolvimento dos estudos da equipe de pesquisa e mais recentemente aprimorado no presente trabalho, batizado de OndisaCAD, integra-se dentro de ambientes CADs, precisamente no AutoCAD da Autodesk, possibilitando, assim, a geração de ótimas interfaces e resultados gráficos. No que tange à dissipação de energia através da vegetação existente nos lagos e suas margens, o aspecto dinâmico associado à própria movimentação da vegetação foi comparado ao comportamento do movimento de vigas engastadas em sua parte inferior, o que permitiu prescrever a movimentação dos organismos vivos (plantas) frente a uma excitação provocada pela passagem de onda / This work continues and perfects an automated model for estimating the height of waves generated in lakes dams, entering the characteristic data of the wind. It follows on the climatology of the winds to determine the largest wave heights and identify critical points, for the safety of navigation and margin of the reservoir. Lakes dams, focus of this dissertation are mostly equipped with aquatic vegetation. Inside this subject, a search for models able to qualify and quantify how the waves generated by winds respond to cross these natural barriers in terms of oscillation of plants, present on the margin, was also discussed. For the purposes set out here, a software was used for predicting waves and structured so that could provide automated graphics results with more accurately and with a shortest possible time. The software, due to the development of studies of the research team and more recently extended in the present work, called OndisaCAD, works within CADs environments, specifically in AutoCAD of Autodesk's, allowing the generation of great interfaces and graphical results. With respect to the dissipating energy through the vegetation in the lakes and their margins, the dynamic aspect associated with their movement of the vegetation was compared to the behavior of the movement of beams embedded in its bottom, which allowed to prescribe the movement of living organisms (plants) front of an excitement caused by the passage of a wave

Orientador: Geraldo de Freitas Maciel / Banca: Carlos Roberto Minussi / Banca: Luiz Edival Souza / Resumo: Este trabalho dá continuidade e aperfeiçoa um modelo automatizado para estimativa de altura de ondas geradas em lagos de barragens, a partir dos dados característicos de vento. Infere sobre a climatologia dos ventos, a fim de determinar as maiores alturas de ondas e identificar pontos críticos, tanto para a segurança à navegação, quanto para as margens do reservatório. Lagos de barragens, foco desta dissertação são, em sua maioria, dotados de vegetação aquática. Dentro dessa temática, uma busca por modelos capazes de qualificar e quantificar o quão as ondas geradas pelo vento reagem ao atravessar esses obstáculos naturais em termos de oscilação das plantas, presentes nas margens, foi também discutida. Para os propósitos aqui expostos, um aplicativo computacional foi utilizado para a previsão de ondas e estruturado de maneira que pudesse fornecer resultados gráficos de forma automatizada com maior precisão e no menor tempo possível. O software, fruto do desenvolvimento dos estudos da equipe de pesquisa e mais recentemente aprimorado no presente trabalho, batizado de OndisaCAD, integra-se dentro de ambientes CADs, precisamente no AutoCAD da Autodesk, possibilitando, assim, a geração de ótimas interfaces e resultados gráficos. No que tange à dissipação de energia através da vegetação existente nos lagos e suas margens, o aspecto dinâmico associado à própria movimentação da vegetação foi comparado ao comportamento do movimento de vigas engastadas em sua parte inferior, o que permitiu prescrever a movimentação dos organismos vivos (plantas) frente a uma excitação provocada pela passagem de onda / Abstract: This work continues and perfects an automated model for estimating the height of waves generated in lakes dams, entering the characteristic data of the wind. It follows on the climatology of the winds to determine the largest wave heights and identify critical points, for the safety of navigation and margin of the reservoir. Lakes dams, focus of this dissertation are mostly equipped with aquatic vegetation. Inside this subject, a search for models able to qualify and quantify how the waves generated by winds respond to cross these natural barriers in terms of oscillation of plants, present on the margin, was also discussed. For the purposes set out here, a software was used for predicting waves and structured so that could provide automated graphics results with more accurately and with a shortest possible time. The software, due to the development of studies of the research team and more recently extended in the present work, called OndisaCAD, works within CADs environments, specifically in AutoCAD of Autodesk's, allowing the generation of great interfaces and graphical results. With respect to the dissipating energy through the vegetation in the lakes and their margins, the dynamic aspect associated with their movement of the vegetation was compared to the behavior of the movement of beams embedded in its bottom, which allowed to prescribe the movement of living organisms (plants) front of an excitement caused by the passage of a wave / Mestre

O dimensionamento das câmaras dissipadoras para válvulas dispersoras demanda um estudo sobre a interação da operação destes elementos, não somente para um ponto de operação, mas também para a faixa operativa do conjunto, que compreende a faixa de operação da válvula e da câmara de dissipação. Os limites sobre responsabilidade assumem um cenário onde as dimensões da câmara podem não ser adequadas à operação da válvula, e vice-versa. Isto porque durante o processo de dissipação de energia, ocorrem grandes turbulências que podem gerar erosão na estrutura dissipadora. A interação entre a operação das válvulas dispersoras e as dimensões da câmara dissipadora é complexa porque o dimensionamento de um elemento está associado ao outro. Assim, as dimensões necessárias para dissipação de energia na câmara dependem de dados da válvula, resultando em uma interdependência de dados para a dissipação de energia adequada. O dimensionamento do conjunto deve levar em consideração a interdependência de operação dos elementos, caso contrário o funcionamento do sistema poderá ser inadequado devido às turbulências e altas velocidades, que podem gerar cavitação e erosão das estruturas dissipadoras. Os danos na estrutura dissipadora podem causar paradas de geração de energia das usinas hidrelétricas e acidentes nas regiões localizadas a jusante desta estrutura. O dimensionamento adequado do conjunto válvula e câmara dissipadora e o conhecimento de sua faixa operativa admissível pode ser feito com auxílio de simulações numéricas e ensaios em modelo reduzido de forma a prever o comportamento adequado do protótipo. Desta forma, as simulações numéricas em CFD possibilitam maior seletividade dos casos que serão ensaiados em modelo reduzido, proporcionando maior assertividade nestes ensaios. / The sizing of valves and chambers for dissipating purpose demands a study about the interaction between these elements, not only from an operation point of view but also the whole operating range of the set, which comprehends the operating range of the valve and the dissipating chamber. The limits of liability assume a scenario where the dimensions of the chamber may be not suitable for operation of the valve, and vice-versa. This is because during dissipating energy process, major turbulences occur which may cause erosion in the dissipating structure. The interaction between the dissipating valve and the dissipating chamber dimensions is complex because the sizing of an element is associated to other. Thus, the required dimensions to dissipate energy on the chamber rely on valve data, resulting in data interdependency required for adequate energy dissipation. The set sizing must consider the operation interdependency of both elements otherwise the system operation may be inadequate due to turbulence high flow velocities, which may cause cavitation and erosion of the dissipating structures. Damages on the dissipating structure may cause energy generation interruption of hydroelectric power plants and accidents on the regions located downstream this structure. The adequate sizing of the set valve and dissipating chamber as well as the information regarding its operating range can be done with the aid of numerical simulations and physical model tests in order to predict the behavior of the prototype. Therefore, numerical simulations in CFD allow more selectivity of the cases which will be tested in a physical model, proportioning higher assertiveness on those tests.

Abstract : Steel and fiber-reinforced-polymer (FRP) materials have different mechanical and physical characteristics. High corrosion resistance, high strength to weight ratio, non-conductivity, favorable fatigue enable the FRP to be considered as alternative reinforcement for structures in harsh environment. Meanwhile, FRP bars have low modulus of elasticity and linear-elastic stress-strain curve. These features raise concerns about the applicability of using such materials as reinforcement for structures prone to earthquakes. The main demand for the structural members in structures subjected to seismic loads is dissipating energy without strength loss which is known as ductility. In the rigid frames, columns are expected to be the primary elements of energy dissipation in structures subjected to seismic loads. The present study addresses the feasibility of reinforced-concrete columns totally reinforced with glass-fiber-reinforced-polymer (GFRP) bars achieving reasonable strength and the drift requirements specified in various codes. Eleven full-scale reinforced concrete columns—two reinforced with steel bars (as reference specimens) and nine totally reinforced with GFRP bars—were constructed and tested to failure. The columns were tested under quasi-static reversed cyclic lateral loading and simultaneously subjected to compression axial load. The columns are 400 mm square cross-section with a shear span 1650 mm. The specimen simulates a column with 3.7 m in height in a typical building with the point of contra-flexure located at the column mid-height. The tested parameters were the longitudinal reinforcement ratio (0.63, 0.95 and 2.14), the spacing of the transverse stirrups (80, 100, 150), tie configuration (C1, C2, C3 and C4), and axial load level (20%, 30% and 40%). The test results clearly show that properly designed and detailed GFRP-reinforced concrete columns could reach high deformation levels with no strength degradation. An acceptable level of energy dissipation compared with steel-reinforced concrete columns is provided by GFRP reinforced concrete columns. The dissipated energy of GFRP reinforced concrete columns was 75% and 70% of the counter steel columns at 2.5% and 4% drift ratio respectively. High drift capacity achieved by the columns up to 10% with no significant loss in strength. The high drift capacity and acceptable dissipated energy enable the GFRP columns to be part of the moment resisting frames in regions prone to seismic activities. The experimental ultimate drift ratios were compared with the estimated drift ratios using the confinement Equation in CSA S806-12. It was found from the comparison that the confinement Equation underestimates values of the drift ratios thus the experimental drift ratios were used to modify transverse FRP reinforcement area in CSA S806-12. The hysteretic behavior encouraged to propose a design procedure for the columns to be part of the moderate ductile and ductile moment resisting frames. The development of design guidelines, however, depends on determining the elastic and inelastic deformations and on assessing the force modification factor and equivalent plastic-hinge length for GFRP-reinforced concrete columns. The experimental results of the GFRP-reinforced columns were used to justify the design guideline, proving the accuracy of the proposed design equations. / L’acier et les matériaux à base de polymères renforcés de fibres (PRF) ont des caractéristiques physiques et mécaniques différentes. La résistance à la haute corrosion, le rapport résistance vs poids, la non-conductivité et la bonne résistance à la fatigue font des barres d’armature en PRF, un renforcement alternatif aux barres d’armature en acier, pour des structures dans des environnements agressifs. Cependant, les barres d’armature en PRF ont un bas module d’élasticité et une courbe contrainte-déformation sous forme linéaire. Ces caractéristiques soulèvent des problèmes d'applicabilité quant à l’utilisation de tels matériaux comme renforcement pour des structures situées en forte zone sismique. La principale exigence pour les éléments structuraux des structures soumises à des charges sismiques est la dissipation d'énergie sans perte de résistance connue sous le nom de ductilité. Dans les structures rigides de type cadre, on s'attend à ce que les colonnes soient les premiers éléments à dissiper l'énergie dans les structures soumises à ces charges. La présente étude traite de la faisabilité des colonnes en béton armé entièrement renforcées de barres d’armature en polymères renforcés de fibres de verre (PRFV), obtenant une résistance et un déplacement latéral raisonnable par rapport aux exigences spécifiées dans divers codes. Onze colonnes à grande échelle ont été fabriquées: deux colonnes renforcées de barres d'acier (comme spécimens de référence) et neuf colonnes renforcées entièrement de barres en PRFV. Les colonnes ont été testées jusqu’à la rupture sous une charge quasi-statique latérale cyclique inversée et soumises simultanément à une charge axiale de compression. Les colonnes ont une section carrée de 400 mm avec une portée de cisaillement de 1650 mm pour simuler une colonne de 3,7 m de hauteur dans un bâtiment typique avec le point d’inflexion situé à la mi-hauteur. Les paramètres testés sont : le taux d’armature longitudinal (0,63%, 0,95% et 2,14 %), l'espacement des étriers (80mm, 100mm, 150 mm), les différentes configurations (C1, C2, C3 et C4) et le niveau de charge axiale (20%, 30 % et 40%). Les résultats des essais montrent clairement que les colonnes en béton renforcées de PRFV et bien conçues peuvent atteindre des niveaux de déformation élevés sans réduction de résistance. Un niveau acceptable de dissipation d'énergie, par rapport aux colonnes en béton armé avec de l’armature en acier, est atteint par les colonnes en béton armé de PRFV. L'énergie dissipée des colonnes en béton armé de PRFV était respectivement de 75% et 70% des colonnes en acier à un rapport déplacement latéral de 2,5% et 4%. Un déplacement supérieur a été atteint par les colonnes en PRFV jusqu'à 10% sans perte significative de résistance. La capacité d’un déplacement supérieur et l’énergie dissipée acceptable permettent aux colonnes en PRFV de participer au moment résistant dans des régions sujettes à des activités sismiques. Les rapports des déplacements expérimentaux ultimes ont été comparés avec les rapports estimés en utilisant l’Équation de confinement du code CSA S806-12. À partir de la comparaison, il a été trouvé que l’Équation de confinement sous-estime les valeurs des rapports de déplacement, donc les rapports de déplacement expérimentaux étaient utilisés pour modifier la zone de renforcement transversal du code CSA S806-12. Le comportement hystérétique encourage à proposer une procédure de conception pour que les colonnes fassent partie des cadres rigides à ductilité modérée et résistant au moment. Cependant, l'élaboration de guides de conception dépend de la détermination des déformations élastiques et inélastiques et de l'évaluation du facteur de modification de la force sismique et de la longueur de la rotule plastique pour les colonnes en béton armé renforcées de PRFV. Les résultats expérimentaux des colonnes renforcées de PRFV étudiées ont été utilisés pour justifier la ligne directrice de conception, ce qui prouve l’efficacité des équations de conception proposées.

L'interaction dynamique sol-structure a été largement explorée en supposant le comportement linéaire du sol. Néanmoins, pour des séismes d'intensité modérée à forte, la contrainte de cisaillement maximale peut facilement atteindre la limite élastique du sol. Du point de vue de l'interaction sol-structure, les effets non linéaires peuvent modifier la rigidité du sol à la base de la structure ainsi que la quantité d'énergie dissipée dans le sol. En conséquence, ignorer les caractéristiques non linéaires du sol dans l'interaction dynamique sol-structure (IDSS) peut conduire à des prédictions erronées de la réponse de la structure. Le but de ce travail est d'implémenter dans un code numérique une loi de comportement non linéaire pour le sol afin d'examiner l'effet de la nonlinéarité du sol sur l'interaction dynamique sol-structure. De plus, différents aspects sont pris en compte tels que l'effet de la contrainte de confinement sur le module de cisaillement du sol, les conditions statiques initiales, les conditions d'interface entre le sol et la structure, etc. Durant ce travail, une méthode simple de couche absorbante basée sur une formulation de Rayleigh / Caughey pour l'amortissement, qui est généralement disponible dans les logiciels existants d'éléments finis, a également été développée. Les conditions de stabilité des problèmes de propagation d'onde sont étudiées et on montre que les comportements linéaire et non linéaire sont très différents en ce qui concerne la dispersion numérique. La règle habituelle de 10 points par longueur d'onde, recommandée dans la littérature pour les milieux élastiques, apparaît pas suffisante dans le cas non linéaire.Le modèle implémenté est d'abord vérifié numériquement en comparant les résultats avec ceux d'autres codes numériques connus. Après cela, une étude paramétrique est menée pour différents types de structures et des profils de sol variés afin de caractériser les effets non linéaires. Différentes caractéristiques de l'IDSS sont comparées à celles du cas linéaire: modification de l'amplitude et du contenu fréquentiel des ondes se propageant dans le sol, fréquence fondamentale, dissipation de l'énergie dans le sol et réponse du système sol-structure. A travers ces études paramétriques nous montrons qu'en fonction des propriétés du sol, le contenu fréquentiel de la réponse du sol peut changer significativement à cause des nonlinéarités de comportement. Les pics de la fonction de transfert entre le champ libre et le rocher affleurant se décalent vers les basses fréquences et l'amplification se produit dans cette gamme de fréquences. Une réduction de l'amplification pour les hautes fréquences et même une dé-amplification peuvent se produire pour un fort niveau des mouvements d'entrée. Ces changements influencent la réponse de la structure. Ce travail montre également que la proximité des fréquences fondamentales de la structure et du sol influence fortement l'interaction sol-structure. Enfin, l'effet du poids de la structure et du balancement de la superstructure peut être significatif. Finalement, le bassin de Nice est utilisé comme un exemple de propagation d'onde dans un milieu non linéaire hétérogène et d'interaction dynamique sol-structure. La réponse du bassin dépend fortement de la combinaison de la nonlinéarité du sol, des effets topographiques et du contraste d'impédance entre les couches de sol. Pour les structures et les profils de sol sélectionnés dans ce travail, les simulations numériques réalisées montrent que le décalage de la fréquence fondamentale n'est pas un bon indicateur pour distinguer le comportement linéaire du sol du comportement non linéaire / The interaction of the soil with the structure has been largely explored the assumption of material and geometrical linearity of the soil. Nevertheless, for moderate or strong seismic events, the maximum shear strain can easily reach the elastic limit of the soil behavior. Considering soil-structure interaction, the nonlinear effects may change the soil stiffness at the base of the structure and therefore energy dissipation into the soil. Consequently, ignoring the nonlinear characteristics of the dynamic soil-structure interaction (DSSI) this phenomenon could lead toerroneous predictions of structural response. The goal of this work is to implement a fully nonlinear constitutive model for soils into anumerical code in order to investigate the effect of soil nonlinearity on dynamic soil structureinteraction. Moreover, different issues are taken into account such as the effect of confining stress on the shear modulus of the soil, initial static condition, contact elements in the soil-structure interface, etc. During this work, a simple absorbing layer method based on a Rayleigh / Caughey damping formulation, which is often already available in existing. Finite Element softwares, is also presented. The stability conditions of the wave propagation problems are studied and it is shown that the linear and nonlinear behavior are very different when dealing with numerical dispersion. It is shown that the 10 points per wavelength rule, recommended in the literature for the elastic media is not sufficient for the nonlinear case. The implemented model is first numerically verified by comparing the results with other known numerical codes. Afterward, a parametric study is carried out for different types of structures and various soil profiles to characterize nonlinear effects. Different features of the DSSI are compared to the linear case : modification of the amplitude and frequency content of the waves propagated into the soil, fundamental frequency, energy dissipation in the soil and the response of the soil-structure system. Through these parametric studies we show that depending on the soil properties, frequency content of the soil response could change significantly due to the soil nonlinearity. The peaks of the transfer function between free field and outcropping responsesshift to lower frequencies and amplification happens at this frequency range. Amplificationreduction for the high frequencies and even deamplication may happen for high level inputmotions. These changes influence the structural response.We show that depending on the combination of the fundamental frequency of the structureand the the natural frequency of the soil, the effect of soil-structure interaction could be significant or negligible. However, the effect of structure weight and rocking of the superstructurecould change the results. Finally, the basin of Nice is used as an example of wave propagation ona heterogeneous nonlinear media and dynamic soil-structure interaction. The basin response isstrongly dependent on the combination of soil nonlinearity, topographic effects and impedancecontrast between soil layers. For the selected structures and soil profiles of this work, the performed numerical simulations show that the shift of the fundamental frequency is not a goodindex to discriminate linear from nonlinear soil behavior