Suppression of the Richtmyer-Meshkov Instability due to a Density Transition Layer at the Interface

TL;DR

This study uses numerical simulations to show that a smooth density transition layer at an interface can suppress the Richtmyer-Meshkov instability when the layer exceeds a certain thickness related to the interface modulation wavelength.

Contribution

It provides an empirical condition for RMI suppression based on the transition layer thickness and introduces a universal feature observed across shock-interface interactions.

Findings

Suppression occurs when the transition layer thickness exceeds the modulation wavelength.

Fluctuation kinetic energy decreases as L^{-2.5}, reducing RMI growth velocity.

Suppression condition relates shock transit time to sound crossing time.

Abstract

We have investigated the effects of a smooth transition layer at the contact discontinuity on the growth of the Richtmyer-Meshkov instability (RMI) by hydrodynamic numerical simulations and derived an empirical condition for the suppression of the instability. The transition layer has little influence on the RMI when the thickness $L$ is narrower than the wavelength of an interface modulation $\lambda$. However, if the transition layer becomes broader than $\lambda$, the perturbed velocity associated with the RMI is reduced considerably. The suppression condition is interpreted as the cases that the shock transit time through the transition layer is longer than the sound crossing time of the modulation wavelength. The fluctuation kinetic energy decreases as $L^{-p}$ with $p = 2.5$, which indicates that the growth velocity of the RMI decreases in proportion to $L^{-p/2}$ by the presence of the transition layer. This feature is found to be quite universal and appeared in a wide range of shock-interface interactions.