The wettability of a surface has been shown, for many years now, to increase by the application of a voltage difference between the liquid droplet and the substrate, 1À3 which, most often, is a conductor covered by a dielectric (electrowetting on the dielectric, EWOD). There are basically two explanations of the phenomenon. The first one considers that the solidÀliquid surface tension is modulated by the electrostatic energy stored by the unit area in the effective capacitance created by the liquid and the substrate. 4 The second explanation considers that there is a net force acting on the electric charge that accumulates at the triple line (TPL) formed among the air, the solid substrate, and the liquid. 5,6 In fact, irrespectively of the explanation given, the contact angle decrease is independent of the polarity of the applied voltage, and the LippmannÀYoung 7 equation for the static contact angle change,has been experimentally demonstrated 8 for a wide range of voltage values prior to a saturation regime. In eq 1, θ 0 is the contact angle before the voltage is applied, θ V is the contact angle after a voltage V is applied, ε 0 is the vacuum permittivity, ε r and d are the relative permittivity and the thickness of the dielectric layer, respectively, and γ LV is the surface tension of the liquidÀgas interface. This increase in wettability contrasts with the decrease in wettability observed after electron bombardment. 9 In a recent paper, 10 we preliminarily discussed a contactless method to increase the wettability by creating the charging conditions of the TPL by air ionization using a corona charge instrument. We are providing in this article a more detailed discussion and systematic measurements of the observations we have made using this technique.Corona ionizers are based on the ionization of molecules of the surrounding air by the application of a sufficiently high potential between specific geometry electrodes (e.g., pin to plane) creating a large electric field gradient. 11 The control of static charge on insulating materials is a widespread use of this technique in the semiconductor industry to avoid undesired electrostatic discharge (ESD). In fact, this is the only practical way to neutralize static charge because grounding has no effect on the level of charge in insulators.In this article, we have used corona ionization to build electrostatic charge on a EWOD structure and analyze the effects this may have on the contact angle between a drop and the surface. Our preliminary experiments reported in ref 10 did show that the contact angle decreased after exposure to corona ionization, and this observation motivated the detailed study of the phenomenon that we report here. There are few works relating electrowetting to air ionization. Vallet et al. 12 attributed to air ionization the saturation phenomena of the contact angle, Blake 13 used a corona charging procedure to assist the study of contact angle change for a constant speed moving substrate, and Arifin et al. 14 investigated the effect of the e...