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Contraction Rate and Its Relationship to Frontogenesis, the Lyapunov Exponent, Fluid Trapping, and Airstream Boundaries

机译:收缩率及其与额生,Lyapunov指数,流体截留和气流边界的关系

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Although a kinematic framework for diagnosing frontogenesis exists in the form of the Petterssen fron-togenesis function and its vector generalization, a similar framework for diagnosing airstream boundaries (e.g., drylines, lee troughs) has not been constructed. This paper presents such a framework, beginning with a kinematic expression for the rate of change of the separation vector between two adjacent air parcels. The maximum growth rate of the separation vector is called the instantaneous dilatation rate and its orientation is called the axis of dilatation. Similarly, a maximum decay rate is called the instantaneous contraction rate and its orientation is called the axis of contraction. These expressions are related to the vector frontogenesis function, in that the growth rate of the separation vector corresponds with the scalar frontogenesis function, and the rotation rate of the separation vector corresponds with the rotational component of the vector frontogenesis function. Because vorticity can rotate air-parcel pairs out of regions of deformation, the instantaneous dilatation and contraction rates and axes may not be appropriate diagnostics of airstream boundaries for fluid flows in general. Rather, the growth rate and orientation of an airstream boundary may correspond better to the so-called asymptotic contraction rate and the asymptotic axis of dilatation, respectively. Expressions for the asymptotic dilatation and contraction rates, as well as their orientations, the asymptotic dilatation and contraction axes, are derived. The asymptotic dilatation rate is related to the Lyapunov exponent for the flow. In addition, a fluid-trapping diagnostic is derived to distinguish among adjacent parcels being pulled apart, being pushed together, or trapped in an eddy. Finally, these diagnostics are applied to simple, idealized, steady-state flows and a nonsteady idealized vortex in nondivergent, diffluent flow to show their utility for determining the character of air-parcel trajectories and airstream boundaries.
机译:尽管以Petterssen子叶形成功能及其矢量概括的形式存在用于诊断前生的运动学框架,但尚未构建用于诊断气流边界(例如,干线,背风槽)的相似框架。本文提出了这样一个框架,从运动学表达式开始,即两个相邻空气小块之间的分离矢量的变化率。分离向量的最大增长率称为瞬时膨胀率,其方向称为膨胀轴。类似地,最大衰减率称为瞬时收缩率,其方向称为收缩轴。这些表达与载体前生功能有关,因为分离载体的生长速率与标量前生功能相对应,分离载体的旋转速率与载体前生功能的旋转分量相对应。由于涡旋可使空气对旋转离开变形区域,因此瞬时膨胀率和收缩率以及轴通常可能不适用于流体流动的气流边界诊断。相反,气流边界的生长速率和取向可以分别更好地对应于所谓的渐近收缩率和扩张的渐近轴。推导了渐进式膨胀率和收缩率及其方向,渐进式膨胀率和收缩轴的表达式。渐近扩张率与流动的李雅普诺夫指数有关。另外,导出了一种流体捕获诊断程序,以区分被拉开,推到一起或陷入涡流中的相邻包裹。最后,这些诊断程序适用于简单,理想化的稳态流动和非发散性,扩散性流动中的非稳态理想化涡流,以显示其在确定航空器轨迹和气流边界特性方面的效用。

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