We investigate the stability of a thin two-dimensional liquid film when a u
niform electric field is applied in a direction parallel to the initially f
lat bounding fluid interfaces. We consider the distinct physical effects of
surface tension and electrically induced forces for an inviscid, incompres
sible nonconducting fluid. The film is assumed to be thin enough and the su
rface forces large enough that gravity can be ignored to leading order. Our
aim is to analyze the nonlinear stability of the flow. We achieve this by
deriving a set of nonlinear evolution equations for the local film thicknes
s and local horizontal velocity. The equations are valid for waves which ar
e long compared to the average film thickness and for symmetrical interfaci
al perturbations. The electric field effects enter nonlocally and the resul
ting system contains a combination of terms which are reminiscent of the Ko
rtweg-de-Vries and the Benjamin-Ono equations. Periodic traveling waves are
calculated and their behavior studied as the electric field increases. Cla
sses of multimodal solutions of arbitrarily small period are constructed nu
merically and it is shown that these are unstable to long wave modulational
instabilities. The instabilities are found to lead to film rupture. We pre
sent extensive simulations that show that the presence of the electric fiel
d causes a nonlinear stabilization of the flow in that it delays singularit
y (rupture) formation. (C) 2001 American Institute of Physics.