1,081 research outputs found

    A numerical model for multigroup radiation hydrodynamics

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    We present in this paper a multigroup model for radiation hydrodynamics to account for variations of the gas opacity as a function of frequency. The entropy closure model (M1) is applied to multigroup radiation transfer in a radiation hydrodynamics code. In difference from the previous grey model, we are able to reproduce the crucial effects of frequency-variable gas opacities, a situation omnipresent in physics and astrophysics. We also account for the energy exchange between neighbouring groups which is important in flows with strong velocity divergence. These terms were computed using a finite volume method in the frequency domain. The radiative transfer aspect of the method was first tested separately for global consistency (reversion to grey model) and against a well established kinetic model through Marshak wave tests with frequency dependent opacities. Very good agreement between the multigroup M1 and kinetic models was observed in all tests. The successful coupling of the multigroup radiative transfer to the hydrodynamics was then confirmed through a second series of tests. Finally, the model was linked to a database of opacities for a Xe gas in order to simulate realistic multigroup radiative shocks in Xe. The differences with the previous grey models are discussed.Comment: 27 pages, 11 figures, Accepted for publication in JQSR

    Global Solutions of the Boltzmann Equation over R D near Global Maxwellians with Small Mass

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    30 pagesWe study the dynamics defined by the Boltzmann equation set in the Euclidean space RD in the vicinity of global Maxwellians with finite mass. A global Maxwellian is a special solution of the Boltzmann equation for which the collision integral vanishes identically. In this setting, the dispersion due to the advection operator quenches the dissipative effect of the Boltzmann collision integral. As a result, the large time limit of solutions of the Boltzmann equation in this regime is given by noninteracting, freely transported states and can be described with the tools of scattering theory

    Finite-time blowup for a complex Ginzburg-Landau equation

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    We prove that negative energy solutions of the complex Ginzburg-Landau equation eiθut=Δu+uαue^{-i\theta} u_t = \Delta u+ |u|^{\alpha} u blow up in finite time, where \alpha >0 and \pi /2<\theta <\pi /2. For a fixed initial value u(0)u(0), we obtain estimates of the blow-up time TmaxθT_{max}^\theta as θ±π/2\theta \to \pm \pi /2 . It turns out that TmaxθT_{max}^\theta stays bounded (respectively, goes to infinity) as θ±π/2\theta \to \pm \pi /2 in the case where the solution of the limiting nonlinear Schr\"odinger equation blows up in finite time (respectively, is global).Comment: 22 page

    Radiative Transfer in Star Formation: Testing FLD and Hybrid Methods

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    We perform a comparison between two radiative transfer algorithms commonly employed in hydrodynamical calculations of star formation: grey flux limited diffusion and the hybrid scheme, in addition we compare these algorithms to results from the Monte-Carlo radiative transfer code MOCASSIN. In disc like density structures the hybrid scheme performs significantly better than the FLD method in the optically thin regions, with comparable results in optically thick regions. In the case of a forming high mass star we find the FLD method significantly underestimates the radiation pressure by a factor of ~100.Comment: 4 Pages; to appear in the proceedings of 'The Labyrinth of Star Formation', Crete, 18-22 June 201

    On the dependence of the Navier Stokes equations on the distribution of moleular velocities

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    In this work we introduce a completely general Chapman Enskog procedure in which we divide the local distribution into an isotropic distribution with anisotropic corrections. We obtain a recursion relation on all integrals of the distribution function required in the derivation of the moment equations. We obtain the hydrodynamic equations in terms only of the first few moments of the isotropic part of an arbitrary local distribution function. The incompressible limit of the equations is completely independent of the form of the isotropic part of the distribution, whereas the energy equation in the compressible case contains an additional contribution to the heat flux. This additional term was also found by Boghosian and by Potiguar and Costa in the derivation of the Navier Stokes equations for Tsallis thermostatistics, and is the only additional term allowed by the Curie principle

    Children’s Mental Health and Emotional Well-being in Primary Schools: A Whole School Approach

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    This text is written for all those working in primary schools and who are involved in supporting children and young people. It supports professionals to develop strategies to enhance the importance of mental health and emotional wellbeing, to work on preventative strategies and to support children when they need more intervention. The text explores what we mean by mental health and wellbeing. It is written for teacher trainees and those studying Child and Adolescent Mental Health

    Generating near-extreme Summer Reference Years (SRY) for building performance simulation

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    Copyright © 2015 by SAGE PublicationsAt present there is no universally accepted method for deriving near-extreme summer weather data for building performance simulation. Existing datasets such as the Design Summer Years (DSY) used in the United Kingdom (UK) to estimate summer discomfort in naturally ventilated and free running buildings have been criticised for being inconsistent with the corresponding Test Reference Years (TRY). This paper proposes a method for generating Summer Reference Years (SRY) by adjusting the TRY of a given site with meteorological data in order to represent near-extreme conditions. It takes as the starting point that the TRY is robust, being determined on a monthly basis from the most typical months. Initial simulations for the 14 UK TRY locations show promising results for determining building overheating with the SRY
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