Abstract

The accelerations of tracer and light particles (bubbles) in compressible homogeneous isotropic turbulence are investigated by using data from direct numerical simulations up to turbulent Mach number $M_t =1$ . For tracer particles, the flatness factor of acceleration components, $F_a$ , increases gradually for $M_t \in [0.3, 1]$ . On the contrary, $F_a$ for bubbles develops a maximum around $M_t \sim 0.6$ . The probability density function of longitudinal acceleration of tracers is increasingly skewed towards the negative value as $M_t$ increases. By contrast, for light particles, the skewness factor of longitudinal acceleration, $S_a$ , first becomes more negative with the increase of $M_t$ , and then goes back to $0$ when $M_t$ is larger than $0.6$ . Similarly, differences among tracers and bubbles appear also in the zero-crossing time of acceleration correlation. It is argued that all these phenomena are intimately linked to the flow structures in the compression regions close to shocklets.

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