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Linear stability of planar premixed flames: reactive Navier-Stokes equations with finite activation energy and arbitrary Lewis number

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Figure 1. (a) Steady solutions in the (T0, Y0)-plane and spatial profiles of (b)temperature, (c) fuel mass fraction and (d) reaction rate, for Q = 4, θ = 70(β = 11.2) and Lewis numbers 0.3 (dashed lines), 1.0 (solid lines) and 1.8 (dot-dashed lines)
Figure 2. Neutral stability boundary in the (l, k)-plane for Pr = 0.75, Q = 5and θ = 70 (β = 9.72)
Figure 3.Dispersion relation for( Pr = 0.75, Q = 5, Le = 1 and θ = 70β = 9.72). Also shown are the SVF (dashed line) and Landau-Darrieus (dottedline) dispersion relations.
Table 1. Comparison of growth rates with those of Denet & Haldenwang (1995)and Fr¨olich & Peyret (1991) for k = 0.20944.
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