LAUSR

It was observed in the first part of this work [C. X. Yu et al., Phys. Rev. E 97, 013102 (2018)2470-004510.1103/PhysRevE.97.013102] that a Rayleigh-Taylor flow with a smoothly varying density at the interface permits a multiplicity of solutions for instability modes. Based on numerical solutions of the eigenvalue problem, a fitting expression for the multiple eigenmodes of the Rayleigh-Taylor instability was provided. However, the fitted curves showed poor agreement with the numerical solutions when the Atwood number was relatively high. This paper develops an asymptotic solution based on the Wentzel-Kramers-Brillouin approximation for high wave numbers in the direction tangential to the interface. The asymptotic solution of the eigenmode of each order can provide a fine prediction for moderate and high wave numbers as confirmed by a comparison with numerical solutions and, more importantly, the physical interpretation of the multiple-mode phenomenon is exhibited. We also show simpler expressions of the growth rates when the Atwood number approaches 0 or 1.