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首页> 外文期刊>Journal of Fluid Mechanics >Nonlinear development of subsonic modes on compressible mixing layers: a unified strongly nonlinear critical-layer theory
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Nonlinear development of subsonic modes on compressible mixing layers: a unified strongly nonlinear critical-layer theory

机译:可压缩混合层上亚音速模式的非线性发展:统一的强非线性临界层理论

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摘要

This paper is concerned with the nonlinear instability of compressible mixing layers in the regime of small to moderate values of Mach number M, in which subsonic modes play a dominant role. At high Reynolds numbers of practical interest, previous Studies have shown that the dominant nonlinear effect controlling the evolution of all instability wave comes from the so-called critical layer. In the incompressible limit (M = 0) the critical-layer dynamics are strongly nonlinear, with the nonlinearity being, associated with the logarithmic singularity of the velocity fluctuation (Goldstein & Leib, J. Fluid Mech. vol. 191, 1988, p. 481). In contrast, in the fully compressible regime (M = O(1)), nonlinearity is associated with a simple-pole singularity in the temperature fluctuation and enters in a weakly nonlinear fashion (Goldstein & Leib, J. Fluid Mech. vol. 207, 1989. p. 73). In this paper, we first consider a weakly compressible regime, corresponding to the distinguished scaling M = O(epsilon(1/4)), for which the strongly nonlinear structure persists but is affected by compressibility at leading order (where epsilon 1 measures the magnitude of the instability mode). A strongly nonlinear system governing the development of the vorticity and temperature perturbation is derived. It is further noted that the strength of the pole singularity is controlled by T-c', the mean temperature gradient at the critical level, and for typical base-flow profiles T-c' is small even when M = O(1). By treating T-c' as an independent parameter of O(epsilon(1/2)), we construct a composite strongly nonlinear theory, from which the weakly nonlinear result for M = O(1) can be derived as all appropriate limiting case. Thus the strongly nonlinear formulation is uniformly valid for O(1) Mach numbers. Numerical solutions show that this theory captures the vortex roll-up process, which remains the most prominent feature of compressible mixing-layer transition. The theory offers an effective tool for investigating the nonlinear instability of mixing layers at high Reynolds numbers.
机译:本文关注可压缩混合层在小至中等Mach值M范围内的非线性不稳定性,其中亚音速模式起主导作用。在具有较高的实际雷诺数时,先前的研究表明,控制所有不稳定性波的演化的主要非线性效应来自所谓的临界层。在不可压缩极限(M = 0)中,临界层动力学是强烈非线性的,非线性与速度波动的对数奇异性有关(Goldstein&Leib,J. Fluid Mech。vol。191,1988,p。 481)。相反,在完全可压缩状态下(M = O(1)),非线性与温度波动中的单极奇异性相关,并以弱非线性方式进入(Goldstein&Leib,J. Fluid Mech。vol.207)。 ,1989年。第73页)。在本文中,我们首先考虑一个弱可压缩状态,对应于显着的标度M = O(epsilon(1/4)),在该状态下,强非线性结构持续存在,但受到超前压缩率的影响(其中epsilon 1测量不稳定模式的大小)。得出了控制涡度和温度扰动发展的强非线性系统。还要注意的是,极点的奇异性受T-c'的控制,临界温度下的平均温度梯度为T-c',对于典型的基本流量分布,T-c'即使在M = O(1)时也很小。通过将T-c'作为O(ε(1/2))的独立参数,我们构建了一个复合的强非线性理论,从中可以得出M = O(1)的弱非线性结果作为所有适当的极限情况。因此,强非线性公式对于O(1)马赫数始终有效。数值解表明,该理论捕获了涡旋卷起过程,该过程仍然是可压缩混合层过渡的最突出特征。该理论为研究高雷诺数下混合层的非线性不稳定性提供了有效的工具。

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