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首页> 外文期刊>Physical review, E. Statistical physics, plasmas, fluids, and related interdisciplinary topics >Decay of passive scalars under the action of single scale smooth velocity fields in bounded two-dimensional domains: From non-self-similar probability distribution functions to self-similar eigenmodes - art. no. 056302
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Decay of passive scalars under the action of single scale smooth velocity fields in bounded two-dimensional domains: From non-self-similar probability distribution functions to self-similar eigenmodes - art. no. 056302

机译:有界二维域中单尺度平滑速度场作用下的无源标量的衰减:从非自相似概率分布函数到自相似本征模-艺术。没有。 056302

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摘要

We examine the decay of passive scalars with small, but nonzero, diffusivity in bounded two-dimensional (2D) domains. The velocity fields responsible for advection are smooth (i.e., they have bounded gradients) and of a single large scale. Moreover, the scale of the velocity field is taken to be similar to the size of the entire domain. The importance of the initial scale of variation of the scalar field with respect to that of the velocity field is strongly emphasized. If these scales are comparable and the velocity field is time periodic, we see the formation of a periodic scalar eigenmode. The eigenmode is numerically realized by means of a deterministic 2D map on a lattice. Analytical justification for the eigenmode is available from theorems in the dynamo literature. Weakening the notion of an eigenmode to mean statistical stationarity, we provide numerical evidence that the eigenmode solution also holds for aperiodic flows (represented by random maps). Turning to the evolution of an initially small scale scalar field, we demonstrate the transition from an evolving (i.e., non-self-similar) probability distribution function (pdf) to a stationary (self-similar) pdf as the scale of variation of the scalar field progresses from being small to being comparable to that of the velocity field (and of the domain). Furthermore, the non-self-similar regime itself consists of two stages. Both stages are examined and the coupling between diffusion and the distribution of the finite time Lyapunov exponents is shown to be responsible for the pdf evolution. [References: 34]
机译:我们在有界二维(2D)域中检查具有较小但非零扩散率的无源标量的衰减。引起对流的速度场是平滑的(即,它们具有有限的梯度)并且具有单个大尺度。而且,速度场的尺度被认为与整个域的大小相似。强烈强调标量场变化的初始尺度相对于速度场的重要性。如果这些比例是可比较的,并且速度场是时间周期的,则我们将看到周期标量本征模的形成。本征模通过格子上的确定性2D映射在数字上实现。本征模态的分析依据可从发电机文献中的定理中获得。将本征模态的概念减弱为表示统计平稳性,我们提供了数值证据,表明本征模态解也适用于非周期性流(由随机映射表示)。关于最初的小规模标量场的演化,我们证明了从演化的(即,非自相似)概率分布函数(pdf)到平稳的(自相似)pdf的转变,是标量场从小到与速度场(和域)的速度相当。此外,非自相似制度本身包括两个阶段。研究了这两个阶段,并证明了扩散与有限时间Lyapunov指数分布之间的耦合是pdf演化的原因。 [参考:34]

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