966 resultados para Velocidade sismica
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Pós-graduação em Desenvolvimento Humano e Tecnologias - IBRC
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OBJETIVO: Avaliar a influência da espessura do osso cortical sobre a velocidade de propagação do ultrassom (in vitro). MÉTODO: Foram utilizadas 60 lâminas ósseas confeccionadas a partir do fêmur de bovinos, com diferentes espessuras, variando de 1 a 6mm (10 de cada). As medidas da velocidade do ultrassom foram realizadas por aparelho projetado para este fim, utilizando técnica subaquática e por contato direto com auxílio de gel de acoplamento. Os transdutores foram posicionados de duas maneiras diferentes; opostos entre si, com o osso entre eles, sendo a medida chamada de transversal; e, paralelos na mesma superfície cortical, sendo a medida chamada de axial. RESULTADOS: Com o modo de transmissão axial, a velocidade de propagação do ultrassom aumenta conforme a espessura do osso cortical aumenta, independente da distância entre os transdutores, até a espessura de 5mm, mantendo-se constante após. Não houve alteração da velocidade quando o modo de transmissão foi transversal. CONCLUSÃO: A velocidade de propagação do ultrassom aumenta com o aumento da espessura da cortical óssea, no modo de transmissão axial, até o momento em que a espessura supera o comprimento da onda, mantendo a velocidade constante a partir de então. Nível de Evidência: Estudo Experimental.
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A estratégia de corrida tem sido apontada como um fator decisivo para o sucesso do atleta. Durante corridas de média e longa duração, a melhor estratégia será aquela capaz de poupar as "reservas fisiológicas", permitindo ao atleta terminar a prova no menor tempo possível. O controle da estratégia de corrida parece ser influenciado por fatores fisiológicos e psicológicos, que são ajustados constantemente durante a corrida, permitindo ao atleta determinar a intensidade do esforço. Diversas variáveis fisiológicas têm sido relacionadas aos ajustes da estratégia de corrida, no entanto, os resultados observados são controversos e foco de grandes discussões. Assim, a presente revisão tem como objetivo propiciar aos profissionais do esporte um melhor entendimento de questões como: 1) quais as melhores estratégias adotadas para determinado tipo de prova?; 2) como os ajustes da estratégia de corrida são realizados?; e 3) quais variáveis fisiológicas influenciam no controle da estratégia de corrida?
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Le strutture caratterizzate da una non coincidenza tra il baricentro delle masse e quello delle rigidezze, chiamate strutture eccentriche, sviluppano degli effetti torsionali se soggette ad un’eccitazione dinamica. Un’accurata analisi delle equazioni del moto di sistemi lineari e non lineari di strutture ad un singolo piano ha portato allo sviluppo di un metodo, detto metodo ALPHA, che, attraverso un parametro, detto parametro “alpha”, permette di stimare gli spostamenti di rotazione in funzione dei soli spostamenti longitudinali. Il limite di questo metodo, tuttavia, è quello di essere riferito a strutture ad un singolo piano, non comuni nella pratica progettuale: si è reso quindi necessario uno studio per testarne la validità anche per strutture multi piano, partendo da strutture semplici a due e tre piani. Data la semplicità del metodo ALPHA, si è deciso di affrontare questo problema cercando di cogliere il comportamento dei diversi piani della struttura multipiano con delle strutture ad un singolo piano. Sono state svolte numerose analisi numeriche in cui sono stati fatti variare i parametri di rigidezza, massa, eccentricità e distribuzione delle rigidezze dei vari piani; come indice di validità della struttura mono piano scelta si è utilizzato il rapporto tra il parametro “psi” dell’i-esimo piano e quello della struttura mono piano scelta, dove “psi” rappresenta il rapporto tra “R” ed “alpha”; “R” è il rapporto tra la massima rotazione e il massimo spostamento longitudinale per una struttura eccentrica soggetta ad un’eccitazione dinamica. Dai risultati ottenuti si deduce che, nella maggioranza dei casi, la struttura mono piano che meglio rappresenta il comportamento di tutti i piani è caratterizzata da massa e rigidezza dell’intera struttura multipiano, da un’eccentricità pari alla minore tra quelle dei vari piani e presenta la peggiore distribuzione delle rigidezze tra quelle che si riscontrano nei vari piani.
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CHAPTER 1:FLUID-VISCOUS DAMPERS In this chapter the fluid-viscous dampers are introduced. The first section is focused on the technical characteristics of these devices, their mechanical behavior and the latest evolution of the technology whose they are equipped. In the second section we report the definitions and the guide lines about the design of these devices included in some international codes. In the third section the results of some experimental tests carried out by some authors on the response of these devices to external forces are discussed. On this purpose we report some technical schedules that are usually enclosed to the devices now available on the international market. In the third section we show also some analytic models proposed by various authors, which are able to describe efficiently the physical behavior of the fluid-viscous dampers. In the last section we propose some cases of application of these devices on existing structures and on new-construction structures. We show also some cases in which these devices have been revealed good for aims that lies outside the reduction of seismic actions on the structures. CHAPTER 2:DESIGN METHODS PROPOSED IN LITERATURE In this chapter the more widespread design methods proposed in literature for structures equipped by fluid-viscous dampers are introduced. In the first part the response of sdf systems in the case of harmonic external force is studied, in the last part the response in the case of random external force is discussed. In the first section the equations of motion in the case of an elastic-linear sdf system equipped with a non-linear fluid-viscous damper undergoing a harmonic force are introduced. This differential problem is analytically quite complex and it’s not possible to be solved in a closed form. Therefore some authors have proposed approximate solution methods. The more widespread methods are based on equivalence principles between a non-linear device and an equivalent linear one. Operating in this way it is possible to define an equivalent damping ratio and the problem becomes linear; the solution of the equivalent problem is well-known. In the following section two techniques of linearization, proposed by some authors in literature, are described: the first technique is based on the equivalence of the energy dissipated by the two devices and the second one is based on the equivalence of power consumption. After that we compare these two techniques by studying the response of a sdf system undergoing a harmonic force. By introducing the equivalent damping ratio we can write the equation of motion of the non-linear differential problem in an implicit form, by dividing, as usual, for the mass of the system. In this way, we get a reduction of the number of variables, by introducing the natural frequency of the system. The equation of motion written in this form has two important properties: the response is linear dependent on the amplitude of the external force and the response is dependent on the ratio of the frequency of the external harmonic force and the natural frequency of the system only, and not on their single values. All these considerations, in the last section, are extended to the case of a random external force. CHAPTER 3: DESIGN METHOD PROPOSED In this chapter the theoretical basis of the design method proposed are introduced. The need to propose a new design method for structures equipped with fluid-viscous dampers arises from the observation that the methods reported in literature are always iterative, because the response affects some parameters included in the equation of motion (such as the equivalent damping ratio). In the first section the dimensionless parameterε is introduced. This parameter has been obtained from the definition of equivalent damping ratio. The implicit form of the equation of motion is written by introducing the parameter ε, instead of the equivalent damping ratio. This new implicit equation of motions has not any terms affected by the response, so that once ε is known the response can be evaluated directly. In the second section it is discussed how the parameter ε affects some characteristics of the response: drift, velocity and base shear. All the results described till this point have been obtained by keeping the non-linearity of the behavior of the dampers. In order to get a linear formulation of the problem, that is possible to solve by using the well-known methods of the dynamics of structures, as we did before for the iterative methods by introducing the equivalent damping ratio, it is shown how the equivalent damping ratio can be evaluated from knowing the value of ε. Operating in this way, once the parameter ε is known, it is quite easy to estimate the equivalent damping ratio and to proceed with a classic linear analysis. In the last section it is shown how the parameter ε could be taken as reference for the evaluation of the convenience of using non-linear dampers instead of linear ones on the basis of the type of external force and the characteristics of the system. CHAPTER 4: MULTI-DEGREE OF FREEDOM SYSTEMS In this chapter the design methods of a elastic-linear mdf system equipped with non-linear fluidviscous dampers are introduced. It has already been shown that, in the sdf systems, the response of the structure can be evaluated through the estimation of the equivalent damping ratio (ξsd) assuming the behavior of the structure elastic-linear. We would to mention that some adjusting coefficients, to be applied to the equivalent damping ratio in order to consider the actual behavior of the structure (that is non-linear), have already been proposed in literature; such coefficients are usually expressed in terms of ductility, but their treatment is over the aims of this thesis and we does not go into further. The method usually proposed in literature is based on energy equivalence: even though this procedure has solid theoretical basis, it must necessary include some iterative process, because the expression of the equivalent damping ratio contains a term of the response. This procedure has been introduced primarily by Ramirez, Constantinou et al. in 2000. This procedure is reported in the first section and it is defined “Iterative Method”. Following the guide lines about sdf systems reported in the previous chapters, it is introduced a procedure for the assessment of the parameter ε in the case of mdf systems. Operating in this way the evaluation of the equivalent damping ratio (ξsd) can be done directly without implementing iterative processes. This procedure is defined “Direct Method” and it is reported in the second section. In the third section the two methods are analyzed by studying 4 cases of two moment-resisting steel frames undergoing real accelerogramms: the response of the system calculated by using the two methods is compared with the numerical response obtained from the software called SAP2000-NL, CSI product. In the last section a procedure to create spectra of the equivalent damping ratio, affected by the parameter ε and the natural period of the system for a fixed value of exponent α, starting from the elasticresponse spectra provided by any international code, is introduced.