A simplified model for coupling Darrieus-Landau and diffusive-thermal instabilities

TL;DR

This paper introduces a simplified model that couples long-wave Darrieus-Landau and short-wave diffusive-thermal instabilities in premixed flames, capturing complex dynamics and cellular structures efficiently.

Contribution

It develops a unified phenomenological framework incorporating a cubic coupling term, revealing new asymptotic regimes and a generalized evolution equation for flame front instabilities.

Findings

Identifies a cubic coupling term in the dispersion relation.

Recovers the Michelson--Sivashinsky equation in certain regimes.

Reveals a DL-DT crossover regime with a nonlocal stabilizing term.

Abstract

A simplified phenomenological model is proposed to couple the long-wave Darrieus--Landau (DL) instability and the short-wave diffusive-thermal (DT) instability in premixed flames. By identifying a cubic coupling term in the linear dispersion relation, representing the leading-order interaction between hydrodynamic expansion and diffusive transport, this framework moves beyond the traditional treatment of these instabilities in isolation. Two distinct asymptotic regimes are identified: the first recovers the classical Michelson--Sivashinsky equation for order-unity positive Markstein numbers $\mathcal M>0$, the second reveals a distinguished DL-DT crossover regime where both instabilities participate at equal order. In this crossover limit, where the Markstein number is small ($\mathcal M \sim \sqrt{\epsilon}$ with $\epsilon$ measuring thermal expansion), a generalized evolution equation is derived featuring a nonlocal stabilising term controlled by the hydro-diffusive number $\mathcal{N} = \mathcal A/\delta_L^2$, where $\mathcal A$ is the hydro-diffusive area -- the characteristic area over which hydrodynamic and diffusive transport processes interact. This term remains active even when Markstein stabilisation vanishes. Numerical solutions in sufficiently large domains based on our model reveal a distinctive chaotic regime in which the characteristic DL cusp structures are in persistent competition with small-scale wrinkles. This minimal unified framework thus captures the essential coupled dynamics governing flame front instability and provides a tractable explanation for the fine-scale cellular structures and accelerated growth rates observed, without recourse to the full complexity of the complete conservation equations.