This paper investigates the non-linear long-wave stability of power-law liq
uid films flow down an inclined plane. The method of long-wave theory is fi
rst used to derive a non-linear evolution equation of film thickness. After
linearizing the non-linear evolution equation, the method of normal mode i
s applied to study its linear stability. Then the method of perturbation wi
th multiple scales is used to solve this non-linear equation. The results r
eveal that the system will be more unstable when power-law exponent n decre
ases. Near the neutral stable state, the subcritical instability and explos
ive solution are possible at small n, and the supercritical and uncondition
al stable region exist only when n exceeds a certain value. Also, decreasin
g the magnitude of n will increase the dimensional wave speed of the unstab
le mode. (C) 2000 Elsevier Science Ltd. All rights reserved.