The influence of hydrodynamic instability on the structure of two-dimension
al (2D) and three-dimensional (3D) cellular flames is numerically investiga
ted. The equation used is the compressible Navier-Stokes equation including
a one-step irreversible chemical reaction. We superimpose an infinitesimal
disturbance on the stationary plane flame and calculate the evolution of t
he disturbed flame front to obtain the relation between the growth rate and
the wave number, i.e., the dispersion relation. With an increase in flame
temperature, the growth rate increases since hydrodynamic instability becom
es stronger. The unstable range normalized by the preheat zone thickness ha
rdly changes, even though the flame temperature increases. The critical wav
e number, which corresponds to the maximum growth rate, is almost constant.
Therefore, the normalized spacing between cells of the cellular flame is i
ndependent of the flame temperature. Moreover, we superimpose the disturban
ce with the critical wave number to investigate the structure of cellular f
lames. The stationary cellular flame is obtained when the inlet-flow veloci
ty is set to the flame velocity of the cellular flame. The higher the flame
temperature, the deeper the cell and the broader the flame surface. In add
ition, the cell depth and the surface area of the 3D flame are larger than
those of the 2D flame. This is caused by the difference in the disposition
of cells. (C) 1999 American Institute of Physics. [S1070-6631(99)00911-3].