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Abstract

The mixing mechanism within a single-vortex has been a theoretical focus for decades, while remains unclear especially under variable-density (VD) scenario. This study investigates canonical single-vortex VD mixing in shock-bubble interactions (SBI) through high-resolution numerical simulations. Special attention is paid to examine the stretching dynamics and its impact on VD mixing within a single-vortex, and this problem is investigated by quantitatively characterizing the scalar dissipation rate (SDR), namely mixing rate, and its time integral, referred to as mixedness. We first examine single-vortex passive-scalar (PS) mixing with the absence of density difference. Under several assumptions, the single-vortex stretching rate illustrates an algebraic growth of the length of scalar strips. By incorporating diffusion process through the solution of the advection-diffusion equation along these stretched strips, a PS mixing model for SDR is proposed. Within this framework, density-gradient effects from two perspectives of stretching dynamics and diffusion process are discovered to challenge the extension of PS mixing model to VD mixing. First, the secondary baroclinic effect increases the VD stretching rate by the additional secondary baroclinic principal strain. Second, the density source effect suppresses the diffusion process. By accounting for both the secondary baroclinic effect on stretching and the density source effect on diffusion, a VD mixing model for SBI is further modified. This model establishes a quantitative relationship between the stretching dynamics and the evolution of the mixing rate and mixedness for single-vortex VD mixing over a broad range of Mach numbers. Furthermore, the essential role of stretching dynamics on the mixing rate is demonstrated by the derived dependence of the time-averaged mixing rate on the Peclet number Pe.