The body-force effect on the lateral movement of cellular flames is studied
by unsteady calculations of reactive flows at low Lewis numbers. We employ
the compressible Navier-Stokes equation including chemical reaction to tak
e account of the hydrodynamic effect caused by thermal expansion. A sinusoi
dal disturbance with the linearly most unstable wavelength is superimposed
on a plane flame to simulate the formation of a cellular flame. The superim
posed disturbance grows initially with time, and then the flame front chang
es from a sinusoidal to a cellular shape. After the cell formation, the cel
lular flame moves laterally at Lewis numbers lower than unity. The reason i
s that the diffusive-thermal effect, and the nonlinear effect of the flame
front, play a primary role in the appearance of the lateral movement of cel
ls. The body-force effect has a great influence on the lateral velocity of
cells. When flames are propagated upward, the lateral velocity decreases as
the acceleration increases, even though the body-force effect has a destab
ilizing influence. When flames are propagated downward, on the other hand,
the lateral velocity takes a maximum value at the specific acceleration and
decreases with an increase in acceleration. The dependence of lateral velo
city on the acceleration is due to the augmentation and diminution in maxim
um flame temperature and to the broadness and narrowness of a high-temperat
ure region behind a convex flame front.