Turbulence Energetics in an Inclined Interface Richtmyer-Meshkov Instability

Akshay Subramaniam, S. Lele
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引用次数: 3

Abstract

The interaction of a Mach 1.55 shockwave with a nominally inclined interface between N2 and CO2 is considered. Unlike the classical Richtmyer-Meshkov problem, the interface evolution is non-linear from early time and large highly correlated vortical structures are observed even after reshock. Simulations target the experiment of McFarland et al. (2014). Simulations are performed using high-order spectral-like numerics (Lele, 1992). Results from multiple grid resolutions up to 4 billion grid points establish grid convergence. Comparisons to the experiments show that the simulations adequately capture the physics of the problem. The turbulence energetics in the problem is investigated using a TKE balance equation based on Favre-averaging and a scale decomposition analysis. Due to the competing time scales of relaxation after compression of the turbulence by the shock and the circulation time scale, a non-monotonic return to isotropy is seen post reshock. TKE budgets are presented and the effect of the dealiasing-filter is quantified and shown to be small (∼ 10%). The budget shows that pressure-dilatation correlation is important even when the turbulent Mach number is ∼ 0.1 (RMS). Scale decomposition shows that the compressibility is due to a complex pattern of shocks and rarefactions created due to the inhomogeneity in the transverse direction and not due to compressible effects in the turbulent mixing region itself. Energetics are investigated at different scales and show that the net flux of energy to smaller scales is scale invariant in the inertial range. Energy injected into the flow due to shocks and rarefactions is seen to be broadband. Finally, the kinetic energy was decomposed into bins in wavenumber space and a k−2 scaling of the energy spectrum was inferred although a larger range of scales could potentially reveal a different scaling at larger wavenumbers.
倾斜界面richmyer - meshkov不稳定性中的湍流能量学
本文考虑了一马赫数为1.55的冲击波与N2和CO2之间名义上的倾斜界面的相互作用。与经典的richmyer - meshkov问题不同的是,界面演化从早期开始就是非线性的,即使在再激波之后也观察到大的高度相关的涡结构。模拟的目标是McFarland et al.(2014)的实验。模拟使用高阶类光谱数值(Lele, 1992)。从多达40亿个网格点的多个网格分辨率得到的结果建立了网格收敛。与实验的比较表明,模拟充分地反映了问题的物理性质。利用基于favre平均和尺度分解分析的TKE平衡方程研究了问题中的湍流能量学。由于激波压缩湍流后的松弛时间尺度与环流时间尺度相竞争,在再激波后出现非单调的向各向同性的回归。给出了TKE预算,并量化了处理滤波器的效果,结果显示效果很小(~ 10%)。预算表明,即使在湍流马赫数为~ 0.1 (RMS)时,压力膨胀相关性也很重要。尺度分解表明,可压缩性是由于激波的复杂模式和横向不均匀性造成的稀疏性,而不是由于湍流混合区域本身的可压缩效应。研究了不同尺度下的能量学,表明在惯性范围内,小尺度的净能量通量是尺度不变的。由于冲击和稀少而注入流中的能量被认为是宽频的。最后,将动能在波数空间中分解为若干个箱子,并推断出能谱的k−2标度,尽管更大的标度范围可能在更大的波数下显示不同的标度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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