Research Article

Effects of Turbulent Reynolds Number on the Displacement Speed Statistics in the Thin Reaction Zones Regime of Turbulent Premixed Combustion

Figure 12

Variation across the flame brush with Favre averaged reaction progress variable ̃ 𝑐 = 𝜌 𝑐 / 𝜌 of the FSD curvature term 2 𝑆 𝑑 𝜅 𝑚 𝑠 Σ g e n and its contributions (see (12c)) 2 ( 𝑆 𝑟 + 𝑆 𝑛 ) 𝜅 𝑚 𝑠 Σ g e n and 4 𝐷 𝜅 2 𝑚 𝑠 Σ g e n ; the FSD propagation term 𝑆 𝑑 𝑁 𝑠 Σ g e n and its contributions (see (12d)) ( 𝑆 𝑟 + 𝑆 𝑛 ) 𝑁 𝑠 Σ g e n and 2 𝐷 𝜅 𝑚 𝑁 𝑠 Σ g e n ; together with the modelled curvature term 2 𝑆 𝐿 𝜅 𝑚 𝑠 Σ g e n and propagation term 𝑆 𝐿 𝑁 𝑠 Σ g e n for: (a) case A; (b) case B; (c) case C; (d) case D; (e) case E. All the terms are normalised with respect to 𝑆 𝐿 / 𝛿 2 t h of the respective cases.
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