It is shown that thin dielectric liquid films between electrically conducti
ng media are dynamically unstable if the electronic work functions of the c
onductors are different. As a consequence, they are expected to dewet by a
spinodal dewetting scenario, i.e., via amplification of surface waves with
mode selection. The wave number of the fastest growing mode is discussed as
a function of the strength of the electric and dispersive forces. In contr
ast to what seems to be widely believed, it turns out that electric forces
dominate over dispersive forces in most experimental situations of the rath
er general type studied here.