Modal model for the nonlinear multimode Rayleigh–Taylor instability

A modal model for the Rayleigh–Taylor (RT) instability, applicable at all stages of the flow, is introduced. The model includes a description of nonlinear low‐order mode coupling, mode growth saturation, and post‐saturation mode coupling. It is shown to significantly extend the range of applicability of a previous model proposed by Haan, to cases where nonlinear mode generation is important. Using the new modal model, we study the relative importance of mode coupling at late nonlinear stages and resolve the difference between cases in which mode generation assumes a dominant role, leading to the late time inverse cascade of modes and loss of memory of initial conditions, and cases where mode generation is not important and memory of initial conditions is retained. Effects of finite density ratios (Atwood number A<1) are also included in the model and the difference between various measures of the mixing zone penetration depth for A<1 is discussed.

[1]  D. Sharp An overview of Rayleigh-Taylor instability☆ , 1984 .

[2]  John Lindl,et al.  Progress toward Ignition and Burn Propagation in Inertial Confinement Fusion , 1992 .

[3]  Stephen E. Bodner,et al.  Rayleigh-Taylor Instability and Laser-Pellet Fusion , 1974 .

[4]  John Lindl,et al.  Hydrodynamic stability and the direct drive approach to laser fusion , 1990 .

[5]  J. Kilkenny,et al.  Laser‐driven hydrodynamic instability experiments* , 1992 .

[6]  D. Hughes,et al.  The nonlinear breakup of a magnetic layer: instability to interchange modes , 1988, Journal of Fluid Mechanics.

[7]  S. Chandrasekhar Hydrodynamic and Hydromagnetic Stability , 1961 .

[8]  S. Haan,et al.  Analysis of weakly nonlinear three‐dimensional Rayleigh–Taylor instability growth , 1995 .

[9]  J. Lindl Development of the indirect‐drive approach to inertial confinement fusion and the target physics basis for ignition and gain , 1995 .

[10]  Hecht,et al.  Scale invariant mixing rates of hydrodynamically unstable interfaces. , 1994, Physical review letters.

[11]  G. Taylor The instability of liquid surfaces when accelerated in a direction perpendicular to their planes. I , 1950, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[12]  U. Alon,et al.  Potential flow models of Rayleigh–Taylor and Richtmyer–Meshkov bubble fronts , 1994 .

[13]  Weber,et al.  Laser-driven planar Rayleigh-Taylor instability experiments. , 1992, Physical review letters.

[14]  Steven A. Orszag,et al.  Three-dimensional simulations and analysis of the nonlinear stage of the Rayleigh-Taylor instability , 1995 .

[15]  Hecht,et al.  Power Laws and Similarity of Rayleigh-Taylor and Richtmyer-Meshkov Mixing Fronts at All Density Ratios. , 1995, Physical review letters.

[16]  Steven A. Orszag,et al.  Nonlinear effects of multifrequency hydrodynamic instabilities on ablatively accelerated thin shells , 1982 .

[17]  S. Haan,et al.  Weakly nonlinear hydrodynamic instabilities in inertial fusion , 1991 .

[18]  K. Nomoto,et al.  Rayleigh-Taylor Instabilities and Mixing in the Helium Star Models for Type Ib/Ic Supernovae , 1991 .

[19]  Sharp,et al.  Chaotic mixing as a renormalization-group fixed point. , 1990, Physical review letters.

[20]  Peter A. Amendt,et al.  Design and modeling of ignition targets for the National Ignition Facility , 1995 .

[21]  D. Youngs,et al.  Modelling turbulent mixing by Rayleigh-Taylor instability , 1989 .

[22]  J. Nuckolls,et al.  Laser Compression of Matter to Super-High Densities: Thermonuclear (CTR) Applications , 1972, Nature.

[23]  J. Dahlburg,et al.  Numerical simulation of ablative Rayleigh–Taylor instability , 1991 .

[24]  D. Youngs,et al.  Numerical simulation of turbulent mixing by Rayleigh-Taylor instability , 1984 .

[25]  S. Sazonov Dissipative structures in the F-region of the equatorial ionosphere generated by Rayleigh-Taylor instability , 1991 .

[26]  Weber,et al.  Multimode Rayleigh-Taylor experiments on Nova. , 1994, Physical review letters.

[27]  Goncharov,et al.  Multiple cutoff wave numbers of the ablative Rayleigh-Taylor instability. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[28]  Haan Onset of nonlinear saturation for Rayleigh-Taylor growth in the presence of a full spectrum of modes. , 1989, Physical review. A, General physics.

[29]  Three-dimensional multimode simulations of the ablative Rayleigh--Taylor instability , 1995 .

[30]  R. Kidder,et al.  Energy gain of laser-compressed pellets: a simple model calculation , 1976 .

[31]  D. Layzer,et al.  On the Instability of Superposed Fluids in a Gravitational Field. , 1955 .

[32]  D. Youngs,et al.  Three-dimensional numerical simulation of turbulent mixing by Rayleigh-Taylor instability , 1991 .

[33]  Uri Alon,et al.  Nonlinear evolution of multimode Rayleigh–Taylor instability in two and three dimensions , 1995 .

[34]  Kunioki Mima,et al.  Self‐consistent growth rate of the Rayleigh–Taylor instability in an ablatively accelerating plasma , 1985 .

[35]  Yamamoto,et al.  Reduction of turbulent mixing at the ablation front of fusion targets. , 1991, Physical review. A, Atomic, molecular, and optical physics.

[36]  I. Catton,et al.  Three-dimensional Rayleigh-Taylor instability Part 1. Weakly nonlinear theory , 1988, Journal of Fluid Mechanics.

[37]  J. D. Kilkenny,et al.  Single‐mode and multimode Rayleigh–Taylor experiments on Nova , 1995 .

[38]  J. Kilkenny,et al.  Large growth, planar Rayleigh–Taylor experiments on Nova , 1992 .

[39]  S. Orszag,et al.  Mode coupling in nonlinear Rayleigh–Taylor instability , 1992 .

[40]  K. I. Read,et al.  Experimental investigation of turbulent mixing by Rayleigh-Taylor instability , 1984 .

[41]  H. Takabe,et al.  Self-consistent eigenvalue analysis of Rayleigh--Taylor instability in an ablating plasma , 1983 .

[42]  J. D. Kilkenny,et al.  A review of the ablative stabilization of the Rayleigh--Taylor instability in regimes relevant to inertial confinement fusion , 1994 .

[43]  Steven A. Orszag,et al.  Two‐phase flow analysis of self‐similar turbulent mixing by Rayleigh–Taylor instability , 1991 .