CEA, DAM, DIF, Bruyères le Châtel, 91297 Arpajon, France.
Philos Trans A Math Phys Eng Sci. 2010 Apr 13;368(1916):1681-704. doi: 10.1098/rsta.2009.0139.
We present a tentative review of compressibility effects in Rayleigh-Taylor instability-induced flows. The linear, nonlinear and turbulent regimes are considered. We first make the classical distinction between the static compressibility or stratification, and the dynamic compressibility owing to the finite speed of sound. We then discuss the quasi-incompressible limits of the Navier-Stokes equations (i.e. the low-Mach number, anelastic and Boussinesq approximations). We also review some results about stratified compressible flows for which instability criteria have been derived rigorously. Two types of modes, convective and acoustic, are possible in these flows. Linear stability results for perfect fluids obtained from an analytical approach, as well as viscous fluid results obtained from numerical approaches, are also reviewed. In the turbulent regime, we introduce Chandrasekhar's observation that the largest structures in the density fluctuations are determined by the initial conditions. The effects of compressibility obtained by numerical simulations in both the nonlinear and turbulent regimes are discussed. The modifications made to statistical models of fully developed turbulence in order to account for compressibility effects are also treated briefly. We also point out the analogy with turbulent compressible Kelvin-Helmholtz mixing layers and we suggest some lines for further investigations.
我们对瑞利-泰勒不稳定性诱导流中的可压缩性效应进行了初步综述。考虑了线性、非线性和湍流等区域。我们首先对静态可压缩性或分层,以及由于声速有限而产生的动态可压缩性进行了经典区分。然后,我们讨论了纳维-斯托克斯方程的拟不可压缩极限(即低马赫数、粘弹性和玻氏近似)。我们还回顾了一些关于分层可压缩流的结果,这些结果已经严格推导出不稳定性准则。在这些流动中,可能存在两种类型的模式,即对流和声波。我们还回顾了从解析方法获得的理想流体线性稳定性结果,以及从数值方法获得的粘性流体结果。在湍流区域,我们引入了 Chandrasekhar 的观察结果,即密度波动中最大的结构由初始条件决定。还讨论了在非线性和湍流区域通过数值模拟获得的可压缩性效应。还简要讨论了为考虑可压缩性效应而对完全发展湍流的统计模型所做的修改。我们还指出了与可压缩的 Kelvin-Helmholtz 混合层的相似性,并提出了一些进一步研究的思路。