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Figure 3 - Direct numerical simulations of temporal compressible mixing layers in a Bethe–Zel'dovich–Thompson dense gas: influence of the convective Mach number

Figure 3. Temporal evolution of the mixing layer momentum thickness for Mc = 0.1/1.1/2.2 using air with PG EoS. Slopes are non-dimensional and standard deviations computed over the self-similar period are indicated on the plot.
Temporal evolution of the mixing layer momentum thickness for Mc = 0.1/1.1/2.2 using air with PG EoS. Slopes are non-dimensional and standard deviations computed over the self-similar period are indicated on the plot.
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