Significance of secondary baroclinic hydrodynamic instability on mixing enhancement in shock-bubble interaction

TL;DR

This study investigates how secondary baroclinic hydrodynamic instability (SBHI) influences mixing in shock-bubble interactions, revealing a proportional relationship between SBHI strength and mixing rate, distinct from high Reynolds number effects.

Contribution

It introduces the SBV number to quantify SBHI strength and demonstrates its significant impact on mixing enhancement, differentiating it from traditional Re-based flow instability.

Findings

Stronger SBHI correlates with higher mixing rates.

Mixing rate scales with the square of SBV numbers.

SBHI effects are distinct from high Re flow instability mechanisms.

Abstract

Different strength of hydrodynamic instability can be induced by the variations in the initial diffusion of shock bubble interaction (SBI), while the influence of hydrodynamic instability on variable-density mixing in SBI remains unclear. The present study aims to investigate the hydrodynamic instability of SBI through high-resolution numerical simulations. To isolate each factor within this instability, a circulation control method is employed to ensure consistent Reynolds number Re and Peclect number Pe. An examination of the morphology of the bubbles and vorticity dynamics reveals that the hydrodynamic instability can be characterized by positive circulation. Through vorticity budget analysis, the positive circulation is dominated by the baroclinic torque. Therefore, the identified hydrodynamic instability is labeled as secondary baroclinic hydrodynamic instability (SBHI). Based on the dimensional analysis of vorticity transport equation, a new dimensionless parameter, the secondary baroclinic vorticity (SBV) number, is proposed to characterize the strength of SBHI. Regarding mixing characteristics, cases with stronger SBHI exhibit higher mixing rates. Indicated by the temporal-averaged mixing rate with different SBV numbers, a scaling behavior is revealed: the mixing rate is increased proportionally to the square of SBV numbers. It is widely recognized that unstable flow can also be induced by a high Reynolds number Re. The distinction and connection of SBHI and high Re unstable flow are further studied. The scaling behavior of the mixing rate in SBHI shows distinct from the Reynolds number Re scaling: the mixing can hardly be altered effectively in the limit of large Re, the mechanisms of which are inherently different with respect to the stretch term, closely relating to the principal strain and the alignment angle between the scalar gradient and the principal strain axis.