1000 resultados para Espalhamento (Fisica)


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Physical Activity produces health! When admitting the precocious veracity that the affirmation introduces, we reconstruct it in ideological dimension to put again the intentions of the physical activity on the scope of the health. To support this displacement, we search endorsement in the concept of Great Health forged in the philosophy of Nietzsche and of this concept we launch considerations about body practices to argue the care from physiological imperatives, worried about the vital necessities of the body. These possibilities only appear when it gave power to the meeting of the subject with himself and with the other - as operated in the body practices context. It is the quality of this meeting that allows trying the Great Health.

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The dance installs in the body another scene of senses that raises the creative performance and not that can be speculated about it. There, ""who dance"" is the Other one, making the body acting of another manner, beyond the systemic contour of Ego. Without the presence of this forged performance, the body would not pass of one ruled machine in function of something and not in favor of himself, as original movement of himself. This article intends to make a reflection about the corporal perception in the dance, trying to point out the creative performance. So, we opened a way to understand the process creative as field of corporal sensitization where the educative intervention is accomplished in the body.

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The study checked possible theory-methodologic assumptions into Physical Education PCNs by the teachers of the last years of elementary school. The analyses in the publishing allow us to identify the different didactic procedures when compared with those which set up the traditional expectations. From these elements and using the projective method, it was developed an interview with focal group. The data obtained showed us docent perceptions which rearrange the educative practice, and interpretation allows us to realize which of the teachers views approaches the propositions in the official document, even if no reference has been done to it.

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The nucleus (46)Ti has been studied with the reaction (42)Ca((7)Li,p2n)(46)Ti at a bombarding energy of 31 MeV. Thin target foils backed with a thick Au layer were used. Five new levels of negative parity were observed. Several lifetimes have been determined with the Doppler shift attenuation method. Low-lying experimental negative-parity levels are assigned to three bands with K(pi) = 3, 0, and 4, which are interpreted in terms of the large-scale shell model, considering particle-hole excitations from d(3/2) and s(1/2) orbitals. Shell model calculations were performed using a few effective interactions. However, good agreement was not achieved in the description of either negative- or positive-parity low-lying levels.

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In the title compound, C(11)H(7)NO(4), there is a dihedral angle of 45.80 (7)degrees between the planes of the benzene and maleimide rings. The presence of O-H...O hydrogen bonding and weak C-H...O interactions allows the formation of R (3) 3(19) edge-connected rings parallel to the (010) plane. Structural, spectroscopic and theoretical studies were carried out. Density functional theory (DFT) optimized structures at the B3LYP/6-311 G(d,p) and 6-31++G(d,p) levels are compared with the experimentally determined molecular structure in the solid state. Additional IR and UV theoretical studies allowed the presence of functional groups and the transition bands of the system to be identified.

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The title compound, C(9)H(8)O(2)S(2), can be used as a chain transfer agent and may be used to control the behavior of polymerization reactions. O-H center dot center dot center dot O hydrogen bonds of moderate character link the molecules into dimers. In the crystal, the dimers are linked into sheets by C-H center dot center dot center dot O interactions, forming R(4)(2)(12) and R(2)(2)(8) edge-fused rings running parallel to [101]. There are no intermolecular interactions involving the S atoms.

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In the title 2:1 adduct, C(14)H(10)O(4)S(2)center dot 0.5C(10)H(8)N(2)O(2), which arose from an unexpected oxidation of a precursor, the dihedral angle between the aromatic rings in the disulfide is 82.51 (11)degrees. In the crystal, the molecules are linked by O-H center dot center dot center dot O, OH center dot center dot center dot N and C-H center dot center dot center dot O interactions, generating sheets.

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We describe the measurement of the depth of maximum, X(max), of the longitudinal development of air showers induced by cosmic rays. Almost 4000 events above 10(18) eV observed by the fluorescence detector of the Pierre Auger Observatory in coincidence with at least one surface detector station are selected for the analysis. The average shower maximum was found to evolve with energy at a rate of (106 +/- 35-21) g/cm(2)/decade below 10(18.24) +/- (0.05) eV, and d24 +/- 3 g/cm(2)/ecade above this energy. The measured shower-to-shower fluctuations decrease from about 55 to 26 g/cm(2). The interpretation of these results in terms of the cosmic ray mass composition is briefly discussed.

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In the title compound, C(3)H(5)N(2)(+)center dot C(4)H(3)O(4)(-), the dihedral angle between the imidazolium ring and the plane formed by the fumarate anion is 80.98 (6)degrees. In the crystal structure, intermolecular O-H center dot center dot center dot O and N-H center dot center dot center dot O hydrogen bonds form extended chains along [100] and [01 (1) over bar], creating a two-dimensional network.

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Data collected at the Pierre Auger Observatory are used to establish an upper limit on the diffuse flux of tau neutrinos in the cosmic radiation. Earth-skimming nu(tau) may interact in the Earth's crust and produce a tau lepton by means of charged-current interactions. The tau lepton may emerge from the Earth and decay in the atmosphere to produce a nearly horizontal shower with a typical signature, a persistent electromagnetic component even at very large atmospheric depths. The search procedure to select events induced by tau decays against the background of normal showers induced by cosmic rays is described. The method used to compute the exposure for a detector continuously growing with time is detailed. Systematic uncertainties in the exposure from the detector, the analysis, and the involved physics are discussed. No tau neutrino candidates have been found. For neutrinos in the energy range 2x10(17) eV < E(nu)< 2x10(19) eV, assuming a diffuse spectrum of the form E(nu)(-2), data collected between 1 January 2004 and 30 April 2008 yield a 90% confidence-level upper limit of E(nu)(2)dN(nu tau)/dE(nu)< 9x10(-8) GeV cm(-2) s(-1) sr(-1).

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In this work, a series of depositions of titanium nitride (TiN) films on M2 and D2 steel substrates were conducted in a Triode Magnetron Sputtering chamber. The temperature; gas flow and pressure were kept constant during each run. The substrate bias was either decreased or increased in a sequence of steps. Residual stress measurements were later conducted through the grazing X-ray diffraction method. Different incident angles were used in order to change the penetration depth and to obtain values of residual stress at different film depths. A model described by Dolle was adapted as an attempt to calculate the values of residual stress at each incident angle as a function of the value from each individual layer. Stress results indicated that the decrease in bias voltage during the deposition has produced compressive residual stress gradients through the film thickness. On the other hand, much less pronounced gradients were found in one of the films deposited with increasing bias voltage. (C) 2010 Elsevier B.V. All rights reserved.

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The present work presents measurements of the Magnetic Barkhausen Noise (MBN) in commercial AISI/SAE 1005 steel samples for different grain sizes. The correlation between the shape of the MBN jump and the grain size is established. The results show the existence of types of MBN jumps. Also, the outcome shows that one of these types of MBN jumps become ""squarer"" with the decrease of grain size.

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The present work shows measurements of the Magnetic Barkhausen Noise (MBN) in commercial AISI/SAE 1045 and ASTM 36 steel deformed samples. The correlation between the MBN root mean square, Barkhausen signal profile and MBN power spectrum with the plastic deformation is established. The results show that the power spectral density of the Barkhausen signal is more effective as nondestructive evaluator than root mean square of Barkhausen signal. The Outcomes also suggest the presence of unbalanced tensions between the surface and the bulk of sample due to the presence of plastic deformation.

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The strange quark matter hypothesis is one of the most exciting speculations of the XX Century Physics. If this hypothesis is correct, the ground state of the matter would be the strange matter, which could form the core of compact objects like neutron stars or even more exotic objects like quarks stars. Due to the high-density and low-temperature regime in these stars, the interaction between quarks through gluon exchange could favor the appearance of a color superconducting state, significantl modifying the equation of state of the system. In this paper we present a general overview of this Subject, taking also into account the effect of strong magnetic field in the quark stars.

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A indústria cimenteira é um dos sectores que mais contribui para um elevado impacto ambiental. O processo de produção de cimento requer a utilização de grandes quantidades de recursos naturais, é energeticamente intensivo e emite elevadas taxas de dióxido de carbono para a atmosfera. Com o presente estudo pretendeu-se contribuir para a mitigação do impacto ambiental provocado pelo processo de fabrico do cimento estudando a viabilidade da substituição parcial de cimento por um material com propriedades cimentícias. O material cimentício estudado foi um resíduo da indústria da refinação de petróleo, em concreto, o catalisador exausto produzido na unidade de “craking” catalítico (FCC) da refinaria da Petrogal, em Sines. Na prossecução do objectivo deste trabalho prepararam-se misturas de cimento com teores de incorporação catalisador exausto de FCC de 5, 10, 15, 20, 25 e 30%, em massa, para avaliar o efeito do teor do resíduo incorporado em propriedades reológicas e mecânicas de argamassas, em função do tempo de hidratação. Pretendeu-se, ainda, avaliar se as misturas de cimento com incorporação do resíduo correspondem às especificações requeridas pela norma europeia em vigor (NP EN 19 -1:2001). Numa segunda fase do trabalho estudou-se ternária composta por cimento, resíduo de catalisador exausto de FCC e resíduo de pedra natural. Em função da sua composição, foram produzidas quatro séries diferentes de argamassas: - Argamassas de referência que incluem na sua composição cimento, areia e água (de acordo com a NP EN 196-1:2006); - Argamassas com substituição parcial de cimento por resíduo de catalisador exausto de FCC tal como foi recebido da refinaria (misturas binárias); - Argamassas com substituição parcial de cimento por resíduo de catalisador exausto de FCC moído (misturas binárias); e, - Argamassas com substituição parcial de cimento por catalisador exausto de FCC e resíduo de pedra natural (misturas ternárias). Todas estas argamassas foram elaboradas adoptando um procedimento experimental que se baseia no descrito na norma NP EN 196-1:2006. Ao longo da campanha experimental, as argamassas foram sujeitas a ensaios no estado fresco e ensaios no estado endurecido, em diferentes tempos de hidratação, para determinar algumas propriedades físicas e mecânicas, respectivamente. As argamassas de referência e as misturas binárias foram ensaiadas aos 2, 7, 28, 56 e 90 dias e as misturas binárias foram ensaiadas aos 2, 7 e 28 dias. No estado fresco realizaram-se ensaios de determinação da consistência por espalhamento, determinação da massa volúmica e ensaios de teor em ar. No estado endurecido foram determinadas as resistências à flexão e à flexão. Da análise dos resultados pod inferir que o resíduo de catalisador exausto de FCC apresenta actividade pozolânica, de tal forma que, argamassas conteores de substituição de cimento por este resíduo até 15% (com adição de superplastificante) estão conforme a norma NP EN 197-1:2001 no que respeita à resistência à compressão, em todos os tempos de hidratação especificados. Relativamente às misturas ternárias, verificou-se que conforme a norma NP EN 197-1:2001, o cimento pode ser substituído pelos dois resíduos em simultâneo até 20%. Verificou-se ainda que utilizando qualquer um dos resíduos com superplastificante, este teor poderia aumentar até 30%.