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The wall-jetting effect in Mach reflection: theoretical consideration and numerical investigation

机译:马赫反射中的壁面喷射效应:理论考虑和数值研究

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The jetting effect often appears in the Mach reflection of a shock and in more complicated irregular shock reflections. It also occurs in some natural phenomena, and industrially important processes. It is studied numerically using a W-modification of the second-order Godunov scheme, to integrate the system of Euler equations. It is shown that there is no correspondence between the shock reflection patterns and the occurrence of jetting. Furthermore, there are two kinds of jetting: strong which occurs when there is a branch point on the ramp surface where the streamlines divide into an upstream moving jet and a downstream moving slug; and weak which has no branch point and may occur at small and large values of the ramp angle theta(omega). The width of the jet for Mach and other reflections is determined by the angle of the Mach stem at the triple point (also called the Mach node or three-shock node). Strong jetting is unstable and the primary instability is in the jet itself. The contact discontinuity is also unstable, but its instability is secondary with respect to the jet instability. Two types of irregular reflection are identified in the dual-solution-domain. They are a two-node system comprising a Mach node followed by a four-shock (overtake) node; and another which seems to be intermediate between the previous system and a three-node reflection, which was first hypothesized by Ben-Dor & Glass (1979). An approximate criterion for the jetting <----> no-jetting transition is presented. It is derived by an analysis of the system of Euler equations for a self-similar flow, and has a simple geometrical interpretation. [References: 31]
机译:喷射效应通常出现在冲击的马赫反射和更复杂的不规则冲击反射中。它也以某些自然现象和工业上重要的过程发生。使用二阶Godunov方案的W修改对它进行数值研究,以集成Euler方程组。结果表明,冲击反射模式与喷射现象之间没有对应关系。此外,有两种喷射:强喷射发生在斜坡表面上的分支点处,流线分为上游移动射流和下游移动弹头。弱且没有分支点,并且可能出现在斜坡角theta(ω)的大小较大和较大的情况下。用于马赫和其他反射的射流的宽度由马赫杆在三点(也称为马赫结或三激波结)处的角度确定。强力喷射不稳定,并且主要不稳定因素在于喷射本身。接触的不连续性也是不稳定的,但是其不稳定性相对于射流不稳定性而言是次要的。在双溶液域中识别出两种类型的不规则反射。它们是一个两节点系统,包括一个马赫节点和一个四冲击(超车)节点。另外一个似乎介于先前系统和三节点反射之间,这是Ben-Dor&Glass(1979)首次提出的假设。提出了喷射<---->无喷射过渡的近似标准。它是通过对自相似流的Euler方程系统进行分析得出的,并且具有简单的几何解释。 [参考:31]

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