998 resultados para FINITE TOTAL CURVATURE


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O crescente nível de degradação das terras tem promovido a adoção de manejos agrícolas que busque aliar a produção agropecuária à conservação do solo. Entre esses, a prática da Integração Lavoura-Pecuária (ILP) tem intensificado-se no Centro-Oeste brasileiro. Com o objetivo de avaliar o efeito em longo prazo do sistema ILP e da sazonalidade, sob a comunidade da macrofauna edáfica e das frações oxidáveis do carbono orgânico total (COT) em áreas de cultivo e Cerradão, foi desenvolvido na Fazenda Cabeceira no município de Maracaju, MS, um estudo em que se mensurou a influência da ILP sobre as frações oxidáveis do COT e sobre a macrofauna edáfica. O sistema ILP está sendo utilizado nessa área desde 2003; o solo foi identificado como Latossolo Vermelho, localizado em área de relevo plano. As áreas amostradas possuem o seguinte histórico: soja/milho + braquiária/algodão/ aveia + pastagem/soja/formação da pastagem/pastagem; as amostragens foram realizadas na época seca, em que as culturas presentes eram pasto, milho+braquiária e algodão; e na chuvosa, com milho+braquiária, algodão e soja. Assim, as áreas nas duas épocas de avaliação foram: pasto/milho, milho+braquiária/ algodão, algodão/soja e uma área nativa de Cerradão. A amostragem foi realizada nas profundidades de 0-10, 10-20 e 20-30 cm, sendo feitas as seguintes determinações: análise da macrofauna edáfica, fracionamento granulométrico da matéria orgânica do solo (MOS) e frações oxidáveis do COT. As áreas não apresentavam delineamento experimental, sendo este um estudo de observação. Os dados foram comparados pelo teste de Kruskal Wallis a 5 % e por meio da análise de redundância. A compartimentalização da MOS pode ser utilizada para a avaliação da qualidade do manejo, sendo os compartimentos mais sensíveis as frações F1 e F2 de frações oxidáveis, pois são mais lábeis no solo, já as frações F3 e F4 são as mais recalcitrantes. Isoptera (cupim) pode estar atuando como agente humificador da matéria orgânica na área de Cerradão, contribuindo para maiores teores de F3 e F4, em relação à F1 e F2 na época seca. Esse padrão somente foi verificado na área de Cerradão, visto que nas áreas de produção, Isoptera é controlado pelo manejo. A falta desse inseto no sistema ILP pode estar reduzindo a estabilização da MOS nas frações F3 e F4.

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BACKGROUND: The association between smoking and total energy expenditure (TEE) is still controversial. We examined this association in a multi-country study where TEE was measured in a subset of participants by the doubly labeled water (DLW) method, the gold standard for this measurement. METHODS: This study includes 236 participants from five different African origin populations who underwent DLW measurements and had complete data on the main covariates of interest. Self-reported smoking status was categorized as either light (<7 cig/day) or high (≥7 cig/day). Lean body mass was assessed by deuterium dilution and physical activity (PA) by accelerometry. RESULTS: The prevalence of smoking was 55% in men and 16% in women with a median of 6.5 cigarettes/day. There was a trend toward lower BMI in smokers than non-smokers (not statistically significant). TEE was strongly correlated with fat-free mass (men: 0.70; women: 0.79) and with body weight (0.59 in both sexes). Using linear regression and adjusting for body weight, study site, age, PA, alcohol intake and occupation, TEE was larger in high smokers than in never smokers among men (difference of 298 kcal/day, p = 0.045) but not among women (162 kcal/day, p = 0.170). The association became slightly weaker in men (254 kcal/day, p = 0.058) and disappeared in women (-76 kcal/day, p = 0.380) when adjusting for fat-free mass instead of body weight. CONCLUSION: There was an association between smoking and TEE among men. However, the lack of an association among women, which may be partly related to the small number of smoking women, also suggests a role of unaccounted confounding factors.

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It is shown that the world volume field theory of a single D3-brane in a supergravity D3-brane background admits finite energy, and non-singular, Abelian monopoles and dyons preserving 1/2 or 1/4 of the N=4 supersymmetry and saturating a Bogomolnyi-type bound. The 1/4 supersymmetric solitons provide a world volume realization of string-junction dyons. We also discuss the dual M-theory realization of the 1/2 supersymmetric dyons as finite tension self-dual strings on the M5-brane, and of the 1/4 supersymmetric dyons as their intersections.

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We derive a Hamiltonian formulation for the three-dimensional formalism of predictive relativistic mechanics. This Hamiltonian structure is used to derive a set of dynamical equations describing the interaction among systems in perturbation theory.

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We explicitly construct a closed system of differential equations describing the electromagnetic and gravitational interactions among bodies to first order in the coupling constants, retaining terms up to order c-2. The Breit and Barker and O'Connell Hamiltonians are recovered by means of a coordinate transformation. The method used throws light on the meaning of these coordinates.

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We compute up to and including all the c-2 terms in the dynamical equations for extended bodies interacting through electromagnetic, gravitational, or short-range fields. We show that these equations can be reduced to those of point particles with intrinsic angular momentum assuming spherical symmetry.

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We study the process of vacuum decay in quantum field theory focusing on the stochastic aspects of the interaction between long- and short-wavelength modes. This interaction results in a diffusive behavior of the reduced Wigner function describing the state of long-wavelength modes, and thereby to a finite activation rate even at zero temperature. This effect can make a substantial contribution to the total decay rate.

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We compute nonequilibrium correlation functions about the stationary state in which the fluid moves as a consequence of tangential stresses on the liquid surface, related to a varying surface tension (thermocapillary motion). The nature of the stationary state makes it necessary to take into account that the system is finite. We then extend a previous analysis on fluctuations about simple stationary states to include some effects related to the finite size of the sample.

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The paper by Woodward [Phys. Rev. A 62, 052105 (2000)] claimed to have proved that Lagrangian theories with a nonlocality of finite extent are necessarily unstable. In this Comment we propose that this conclusion is false.

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We have shown that finite-size effects in the correlation functions away from equilibrium may be introduced through dimensionless numbers: the Nusselt numbers, accounting for both the nature of the boundaries and the size of the system. From an analysis based on fluctuating hydrodynamics, we conclude that the mean-square fluctuations satisfy scaling laws, since they depend only on the dimensionless numbers in addition to reduced variables. We focus on the case of diffusion modes and describe some physical situations in which finite-size effects may be relevant.

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A dynamical model based on a continuous addition of colored shot noises is presented. The resulting process is colored and non-Gaussian. A general expression for the characteristic function of the process is obtained, which, after a scaling assumption, takes on a form that is the basis of the results derived in the rest of the paper. One of these is an expansion for the cumulants, which are all finite, subject to mild conditions on the functions defining the process. This is in contrast with the Lévy distribution¿which can be obtained from our model in certain limits¿which has no finite moments. The evaluation of the spectral density and the form of the probability density function in the tails of the distribution shows that the model exhibits a power-law spectrum and long tails in a natural way. A careful analysis of the characteristic function shows that it may be separated into a part representing a Lévy process together with another part representing the deviation of our model from the Lévy process. This