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首页> 外文期刊>Bulletin of the American Physical Society >APS -70th Annual Meeting of the APS Division of Fluid Dynamics- Event - Upper bounds on the heat flux in 2D Rayleigh-Bénard convection using a 2D background field method
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APS -70th Annual Meeting of the APS Division of Fluid Dynamics- Event - Upper bounds on the heat flux in 2D Rayleigh-Bénard convection using a 2D background field method

机译:APS-流体动力学APS分部第70届年会-事件-使用2D背景场方法在2DRayleigh-Bénard对流中的热通量上限

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The background method [1] has proved a popular and effective technique for estimating the maximal heat flux possible in turbulent Rayleigh-Benard convection. In this method, the temperature is non-uniquely decomposed into a background field which satisfies the physical boundary conditions and a fluctuation field satisfying homogenous boundary conditions. So far, only a 1D background field (just varying with the wall normal direction) has been studied which has the effect of only imposing the horizontal average of the heat equation as a constraint [2]. Here we consider a 2D background field, which imposes the full heat equation, to bound the heat flux in 2D Rayleigh-Benard convection. The results of applying a time-stepping method, which has recently proved successful for the 1D background field case [3], to the extended variational problem will be discussed.References[1] C. R. Doering {&} P. Constantin, Phys. Rev. Lett., extbf{69}, 1648-1651, (1992)[2] C. R. Doering {&} P. Constantin, Phys. Rev. E, extbf{53}, 5957-5981 (1996)[3] B. Wen, G.P. Chini, R.R. Kerswell and C.R. Doering, Phys. Rev. E. extbf{92 }043012 (2015)
机译:背景方法[1]已证明是一种流行的有效技术,用于估计湍流瑞利-贝纳德对流中的最大热通量。在该方法中,温度被非唯一地分解为满足物理边界条件的背景场和满足均匀边界条件的波动场。到目前为止,仅研究了一维背景场(随壁法线方向变化),其效果仅是将热量方程的水平平均值作为约束条件[2]。在这里,我们考虑一个2D背景场,该场强加了完整的热量方程,以限制2D Rayleigh-Benard对流中的热通量。讨论了将时间步进方法应用于扩展的变分问题的方法,该方法最近在一维背景场的情况下[3]成功,将得到讨论。参考文献[1]。C. R. Doering {&} P. Constantin,Phys。 Rev.Lett。,extbf {69},1648-1651,(1992)[2] C.R.Doering {&} P.Constantin,Phys。修订版E,extbf {53},5957-5981(1996)[3] B. Wen,G.P. Chini,R.R. Kerswell和C.R. Doering,Phys。 Rev.E. extbf {92} 043012(2015)

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