16,600 research outputs found

    Influência do preparo do solo nas perdas de água de chuva na cultura do milho.

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    Os diferentes sistemas de preparo dos solos utilizados pelos agricultores no Semi-Árido brasileiro apresentam situações diversas quanto ao aproveitamento da água para as culturas exploradas em condições dependentes de chuva. Neste trabalho, objetivou-se avaliar as perdas de água escoada de uma área submetida a diferentes sistemas de preparo do solo, cultivada com milho (Zea mays L.), correspondendo a T1 (Guimarães Duque); T2 (Aração profunda); T3 (Aração parcial); T4 (Sulcos barrados) e T5 (Sistema tradicional), que corresponde ao plantio no plano. A análise dos resultados referentes aos tratamentos apresenta que o T1 proporcionou maior volume de água escoado no ciclo da cultura (6.696 L), superando a testemunha (T5) que foi de 5.163,3 L. Por outro lado, o menor volume escoado ocorreu no tratamento com sulcos barrados (T4) que correspondeu a 1.066 L no mesmo período. Neste tratamento (T4) também foram obtidas as maiores produtividades de grão da cultura do milho (606 kg ha-1)

    Scattering and self-adjoint extensions of the Aharonov-Bohm hamiltonian

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    We consider the hamiltonian operator associated with planar sec- tions of infinitely long cylindrical solenoids and with a homogeneous magnetic field in their interior. First, in the Sobolev space H2\mathcal H^2, we characterize all generalized boundary conditions on the solenoid bor- der compatible with quantum mechanics, i.e., the boundary conditions so that the corresponding hamiltonian operators are self-adjoint. Then we study and compare the scattering of the most usual boundary con- ditions, that is, Dirichlet, Neumann and Robin.Comment: 40 pages, 5 figure

    Energy of general 4-dimensional stationary axisymmetric spacetime in the teleparallel geometry

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    The field equation with the cosmological constant term is derived and the energy of the general 4-dimensional stationary axisymmetric spacetime is studied in the context of the hamiltonian formulation of the teleparallel equivalent of general relativity (TEGR). We find that, by means of the integral form of the constraints equations of the formalism naturally without any restriction on the metric parameters, the energy for the asymptotically flat/de Sitter/Anti-de Sitter stationary spacetimes in the Boyer-Lindquist coordinate can be expressed as E=18πSdθdϕ(sinθgθθ+gϕϕ(1/grr)(gθθgϕϕ/r))E=\frac{1}{8\pi}\int_S d\theta d\phi(sin\theta \sqrt{g_{\theta\theta}}+\sqrt{g_{\phi\phi}}-(1/\sqrt{g_{rr}})(\partial{\sqrt{g_ {\theta\theta} g_{\phi\phi}}}/\partial r)). It is surprised to learn that the energy expression is relevant to the metric components grrg_{rr}, gθθg_{\theta\theta} and gϕϕg_{\phi\phi} only. As examples, by using this formula we calculate the energies of the Kerr-Newman (KN), Kerr-Newman Anti-de Sitter (KN-AdS), Kaluza-Klein, and Cveti\v{c}-Youm spacetimes.Comment: 12 page

    Gravitational Lorentz Force and the Description of the Gravitational Interaction

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    In the context of a gauge theory for the translation group, we have obtained, for a spinless particle, a gravitational analog of the Lorentz force. Then, we have shown that this force equation can be rewritten in terms of magnitudes related to either the teleparallel or the riemannian structures induced in spacetime by the presence of the gravitational field. In the first case, it gives a force equation, with torsion playing the role of force. In the second, it gives the usual geodesic equation of General Relativity. The main conclusion is that scalar matter is able to feel anyone of the above spacetime geometries, the teleparallel and the metric ones. Furthermore, both descriptions are found to be completely equivalent in the sense that they give the same physical trajectory for a spinless particle in a gravitational field.Comment: Equations (44)-(47) correcte

    Teleparallel Spin Connection

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    A new expression for the spin connection of teleparallel gravity is proposed, given by minus the contorsion tensor plus a zero connection. The corresponding minimal coupling is covariant under local Lorentz transformation, and equivalent to the minimal coupling prescription of general relativity. With this coupling prescription, therefore, teleparallel gravity turns out to be fully equivalent to general relativity, even in the presence of spinor fields.Comment: 2 pages, RevTeX, to appear in Phys. Rev D (Brief Report

    A New Spin Foam Model for 4d Gravity

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    Starting from Plebanski formulation of gravity as a constrained BF theory we propose a new spin foam model for 4d Riemannian quantum gravity that generalises the well-known Barrett-Crane model and resolves the inherent to it ultra-locality problem. The BF formulation of 4d gravity possesses two sectors: gravitational and topological ones. The model presented here is shown to give a quantization of the gravitational sector, and is dual to the recently proposed spin foam model of Engle et al. which, we show, corresponds to the topological sector. Our methods allow us to introduce the Immirzi parameter into the framework of spin foam quantisation. We generalize some of our considerations to the Lorentzian setting and obtain a new spin foam model in that context as well.Comment: 40 pages; (v2) published versio
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