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. Author manuscript; available in PMC: 2019 Oct 19.
Published in final edited form as: Annu Rev Fluid Mech. 2018 Jan;50:535–561. doi: 10.1146/annurev-fluid-122316-045241

Figure 6.

Figure 6

(a) Skin friction coefficient predictions for an H-type transitional boundary layer. The red solid line represents a nonequilibrium wall model (Park & Moin 2014), the dark yellow dashed line represents a DNS of H-type transition (Sayadi et al. 2013), the magenta dashed line with dots represents a DNS of bypass transition (Wu & Moin 2009), the orange line with long dashes represents a WRLES (Schlatter et al. 2010), and the gray circles represent the empirical correlation (Fernholz & Finley 1996). Adapted from Park & Moin (2014). (b) Skin friction coefficient predictions for an oblique shock/boundary-layer interaction at Ma = 1.7, β = 6°. The blue solid line represents a nonequilibrium wall model with linear κ(y) (Kawai & Larsson 2013), the purple dashed line represents a nonequilibrium wall model with constant κ = 0.4 (Balaras et al. 1996), and the gray circles represent the experiment (Souverein et al. 2010). Adapted from Kawai & Larsson (2013). Abbreviations: DNS, direct numerical simulation; WRLES, wall-resolved large-eddy simulation.