  The nonlocal Kuramoto-Sivashinsky equation arises in the modeling of the flow
of a thin film of viscous liquid falling down an inclined plane, subject to an
applied electric field. In this paper, the authors show that, as the
coefficient of the nonlocal integral term goes to zero, the solution
trajectories and the maximal attractor of the nonlocal Kuramoto-Sivashinsky
equation converge to those of the usual Kuramoto-Sivashinsky equation.
